Optical image capturing system

ABSTRACT

An optical image capturing system includes, along the optical axis in order from an object side to an image side, a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, and a seventh lens. At least one lens among the first to the sixth lenses has positive refractive force. The seventh lens can have negative refractive force, wherein both surfaces thereof are aspheric, and at least one surface thereof has an inflection point. The lenses in the optical image capturing system which have refractive power include the first to the seventh lenses. The optical image capturing system can increase aperture value and improve the imagining quality for use in compact cameras.

The current application claims a foreign priority to application number 104141305 filed on Dec. 9, 2015 in Taiwan.

BACKGROUND OF THE INVENTION 1. Technical Field

The present invention relates generally to an optical system, and more particularly to a compact optical image capturing system for an electronic device.

2. Description of Related Art

In recent years, with the rise of portable electronic devices having camera functionalities, the demand for an optical image capturing system is raised gradually. The image sensing device of the ordinary photographing camera is commonly selected from charge coupled device (CCD) or complementary metal-oxide semiconductor sensor (CMOS Sensor). In addition, as advanced semiconductor manufacturing technology enables the minimization of the pixel size of the image sensing device, the development of the optical image capturing system towards the field of high pixels. Therefore, the requirement for high imaging quality is rapidly raised.

The conventional optical system of the portable electronic device usually has five or six lenses. However, the optical system is asked to take pictures in a dark environment, in other words, the optical system is asked to have a large aperture. The conventional optical system provides high optical performance as required.

It is an important issue to increase the quantity of light entering the lens. In addition, the modern lens is also asked to have several characters, including high image quality.

BRIEF SUMMARY OF THE INVENTION

The aspect of embodiment of the present disclosure directs to an optical image capturing system and an optical image capturing lens which use combination of refractive powers, convex and concave surfaces of seven-piece optical lenses (the convex or concave surface in the disclosure denotes the geometrical shape of an image-side surface or an object-side surface of each lens on an optical axis) to increase the quantity of incoming light of the optical image capturing system, and to improve imaging quality for image formation, so as to be applied to minimized electronic products.

The term and its definition to the lens parameter in the embodiment of the present are shown as below for further reference.

The lens parameter related to a length or a height in the lens:

A maximum height for image formation of the optical image capturing system is denoted by HOI. A height of the optical image capturing system is denoted by HOS. A distance from the object-side surface of the first lens to the image-side surface of the seventh lens is denoted by InTL. A distance from the first lens to the second lens is denoted by IN12 (instance). A central thickness of the first lens of the optical image capturing system on the optical axis is denoted by TP1 (instance).

The lens parameter related to a material in the lens:

An Abbe number of the first lens in the optical image capturing system is denoted by NA1 (instance). A refractive index of the first lens is denoted by Nd1 (instance).

The lens parameter related to a view angle in the lens:

A view angle is denoted by AF. Half of the view angle is denoted by HAF. A major light angle is denoted by MRA.

The lens parameter related to exit/entrance pupil in the lens:

An entrance pupil diameter of the optical image capturing system is denoted by HEP. For any surface of any lens, a maximum effective half diameter (EHD) is a perpendicular distance between an optical axis and a crossing point on the surface where the incident light with a maximum viewing angle of the system passing the very edge of the entrance pupil. For example, the maximum effective half diameter of the object-side surface of the first lens is denoted by EHD11, the maximum effective half diameter of the image-side surface of the first lens is denoted by EHD12, the maximum effective half diameter of the object-side surface of the second lens is denoted by EHD21, the maximum effective half diameter of the image-side surface of the second lens is denoted by EHD22, and so on.

The lens parameter related to an arc length of the shape of a surface and a surface profile:

For any surface of any lens, a profile curve length of the maximum effective half diameter is, by definition, measured from a start point where the optical axis of the belonging optical image capturing system passes through the surface of the lens, along a surface profile of the lens, and finally to an end point of the maximum effective half diameter thereof. In other words, the curve length between the aforementioned start and end points is the profile curve length of the maximum effective half diameter, which is denoted by ARS. For example, the profile curve length of the maximum effective half diameter of the object-side surface of the first lens is denoted by ARS11, the profile curve length of the maximum effective half diameter of the image-side surface of the first lens is denoted by ARS12, the profile curve length of the maximum effective half diameter of the object-side surface of the second lens is denoted by ARS21, the profile curve length of the maximum effective half diameter of the image-side surface of the second lens is denoted by ARS22, and so on.

For any surface of any lens, a profile curve length of a half of the entrance pupil diameter (HEP) is, by definition, measured from a start point where the optical axis of the belonging optical image capturing system passes through the surface of the lens, along a surface profile of the lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis. In other words, the curve length between the aforementioned stat point and the coordinate point is the profile curve length of a half of the entrance pupil diameter (HEP), and is denoted by ARE. For example, the profile curve length of a half of the entrance pupil diameter (HEP) of the object-side surface of the first lens is denoted by ARE11, the profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the first lens is denoted by ARE12, the profile curve length of a half of the entrance pupil diameter (HEP) of the object-side surface of the second lens is denoted by ARE21, the profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the second lens is denoted by ARE22, and so on.

The lens parameter related to a depth of the lens shape:

A distance in parallel with the optical axis from a point where the optical axis passes through to an end point of the maximum effective semi diameter on the object-side surface of the seventh lens is denoted by InRS71 (the depth of the maximum effective semi diameter). A distance in parallel with the optical axis from a point where the optical axis passes through to an end point of the maximum effective semi diameter on the image-side surface of the seventh lens is denoted by InRS72 (the depth of the maximum effective semi diameter). The depth of the maximum effective semi diameter (sinkage) on the object-side surface or the image-side surface of any other lens is denoted in the same manner.

The lens parameter related to the lens shape:

A critical point C is a tangent point on a surface of a specific lens, and the tangent point is tangent to a plane perpendicular to the optical axis and the tangent point cannot be a crossover point on the optical axis. Following the above description, a distance perpendicular to the optical axis between a critical point C51 on the object-side surface of the fifth lens and the optical axis is HVT51 (instance), and a distance perpendicular to the optical axis between a critical point C52 on the image-side surface of the fifth lens and the optical axis is HVT52 (instance). A distance perpendicular to the optical axis between a critical point C61 on the object-side surface of the sixth lens and the optical axis is HVT61 (instance), and a distance perpendicular to the optical axis between a critical point C62 on the image-side surface of the sixth lens and the optical axis is HVT62 (instance). A distance perpendicular to the optical axis between a critical point on the object-side or image-side surface of other lenses, such as the seventh lens, and the optical axis is denoted in the same manner.

The object-side surface of the seventh lens has one inflection point IF711 which is nearest to the optical axis, and the sinkage value of the inflection point IF711 is denoted by SGI711 (instance). A distance perpendicular to the optical axis between the inflection point IF711 and the optical axis is HIF711 (instance). The image-side surface of the seventh lens has one inflection point IF721 which is nearest to the optical axis, and the sinkage value of the inflection point IF721 is denoted by SGI721 (instance). A distance perpendicular to the optical axis between the inflection point IF721 and the optical axis is HIF721 (instance).

The object-side surface of the seventh lens has one inflection point IF712 which is the second nearest to the optical axis, and the sinkage value of the inflection point IF712 is denoted by SGI712 (instance). A distance perpendicular to the optical axis between the inflection point IF712 and the optical axis is HIF712 (instance). The image-side surface of the seventh lens has one inflection point IF722 which is the second nearest to the optical axis, and the sinkage value of the inflection point IF722 is denoted by SGI722 (instance). A distance perpendicular to the optical axis between the inflection point IF722 and the optical axis is HIF722 (instance).

The object-side surface of the seventh lens has one inflection point IF713 which is the third nearest to the optical axis, and the sinkage value of the inflection point IF713 is denoted by SGI713 (instance). A distance perpendicular to the optical axis between the inflection point IF713 and the optical axis is HIF713 (instance). The image-side surface of the seventh lens has one inflection point IF723 which is the third nearest to the optical axis, and the sinkage value of the inflection point IF723 is denoted by SGI723 (instance). A distance perpendicular to the optical axis between the inflection point IF723 and the optical axis is HIF723 (instance).

The object-side surface of the seventh lens has one inflection point IF714 which is the fourth nearest to the optical axis, and the sinkage value of the inflection point IF714 is denoted by SGI714 (instance). A distance perpendicular to the optical axis between the inflection point IF714 and the optical axis is HIF714 (instance). The image-side surface of the seventh lens has one inflection point IF724 which is the fourth nearest to the optical axis, and the sinkage value of the inflection point IF724 is denoted by SGI724 (instance). A distance perpendicular to the optical axis between the inflection point IF724 and the optical axis is HIF724 (instance).

An inflection point, a distance perpendicular to the optical axis between the inflection point and the optical axis, and a sinkage value thereof on the object-side surface or image-side surface of other lenses is denoted in the same manner.

The lens parameter related to an aberration:

Optical distortion for image formation in the optical image capturing system is denoted by ODT. TV distortion for image formation in the optical image capturing system is denoted by TDT. Further, the range of the aberration offset for the view of image formation may be limited to 50%-100% field. An offset of the spherical aberration is denoted by DFS. An offset of the coma aberration is denoted by DFC.

Transverse aberration on an edge of an aperture is denoted by STA, which stands for STOP transverse aberration, and is used to evaluate the performance of one specific optical image capturing system. The transverse aberration of light in any field of view can be calculated with a tangential fan or a sagittal fan. More specifically, the transverse aberration caused when the longest operation wavelength (e.g., 650 nm) and the shortest operation wavelength (e.g., 470 nm) pass through the edge of the aperture can be used as the reference for evaluating performance. The coordinate directions of the aforementioned tangential fan can be further divided into a positive direction (upper light) and a negative direction (lower light). The longest operation wavelength which passes through the edge of the aperture has an imaging position on the image plane in a particular field of view, and the reference wavelength of the mail light (e.g., 555 nm) has another imaging position on the image plane in the same field of view. The transverse aberration caused when the longest operation wavelength passes through the edge of the aperture is defined as a distance between these two imaging positions. Similarly, the shortest operation wavelength which passes through the edge of the aperture has an imaging position on the image plane in a particular field of view, and the transverse aberration caused when the shortest operation wavelength passes through the edge of the aperture is defined as a distance between the imaging position of the shortest operation wavelength and the imaging position of the reference wavelength. The performance of the optical image capturing system can be considered excellent if the transverse aberrations of the shortest and the longest operation wavelength which pass through the edge of the aperture and image on the image plane in 0.7 field of view (i.e., 0.7 times the height for image formation HOI) are both less than 100 μm. Furthermore, for a stricter evaluation, the performance cannot be considered excellent unless the transverse aberrations of the shortest and the longest operation wavelength which pass through the edge of the aperture and image on the image plane in 0.7 field of view are both less than 80 μm.

The optical image capturing system has a maximum image height HOI on the image plane vertical to the optical axis. A transverse aberration at 0.7 HOI in the positive direction of the tangential fan after the longest operation wavelength of visible light passing through the edge of the aperture is denoted by PLTA; a transverse aberration at 0.7 HOI in the positive direction of the tangential fan after the shortest operation wavelength of visible light passing through the edge of the aperture is denoted by PSTA; a transverse aberration at 0.7 HOI in the negative direction of the tangential fan after the longest operation wavelength of visible light passing through the edge of the aperture is denoted by NLTA; a transverse aberration at 0.7 HOI in the negative direction of the tangential fan after the shortest operation wavelength of visible light passing through the edge of the aperture is denoted by NSTA; a transverse aberration at 0.7 HOI of the sagittal fan after the longest operation wavelength of visible light passing through the edge of the aperture is denoted by SLTA; a transverse aberration at 0.7 HOI of the sagittal fan after the shortest operation wavelength of visible light passing through the edge of the aperture is denoted by SSTA.

The present invention provides an optical image capturing system capable of focusing for both visible light and infrared light (i.e., dual mode) with certain performance, in which the seventh lens is provided with an inflection point at the object-side surface or at the image-side surface to adjust the incident angle of each view field and modify the ODT and the TDT. In addition, the surfaces of the seventh lens are capable of modifying the optical path to improve the imagining quality.

The optical image capturing system of the present invention includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and an image plane in order along an optical axis from an object side to an image side. The first lens has refractive power. The optical image capturing system satisfies:

1.0≦f/HEP≦10.0; 0 deg<HAF≦150 deg; and 0.9≦2(ARE/HEP)≦1.5;

where f1, f2, f3, f4, f5, f6, and f7 are respectively the focal lengths of the first lens to the seventh lens; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HOS is a distance in parallel with the optical axis between an object-side surface, which face the object side, of the first lens and the image plane; InTL is a distance between the object-side surface of the first lens and the image-side surface of the seventh lens on the optical axis; HAF is a half of the maximum field angle; ARE is a profile curve length measured from a start point where the optical axis of the belonging optical image capturing system passes through the surface of the lens, along a surface profile of the lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis.

The present invention further provides an optical image capturing system, including a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and an image plane in order along an optical axis from an object side to an image side. The first lens has refractive power. The second lens has refractive power. The third lens has refractive power. The fourth lens has refractive power. The fifth lens has refractive power. The sixth lens has refractive power. The seventh lens has refractive power, wherein the object-side surface and the image-side surface thereof are both aspheric surfaces. Each of at least two lenses among the first lens to the seventh lens has at least an inflection point on at least a surface thereof. The optical image capturing system satisfies:

1.0≦f/HEP≦10.0; 0 deg<HAF≦150 deg; and 0.9≦2(ARE/HEP)≦1.5;

where f1, f2, f3, f4, f5, f6, and f7 are respectively the focal lengths of the first lens to the seventh lens; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HOS is a distance in parallel with the optical axis between an object-side surface, which face the object side, of the first lens and the image plane; InTL is a distance between the object-side surface of the first lens and the image-side surface of the seventh lens on the optical axis; HAF is a half of the maximum field angle; ARE is a profile curve length measured from a start point where the optical axis of the belonging optical image capturing system passes through the surface of the lens, along a surface profile of the lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis.

The present invention further provides an optical image capturing system, including a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and an image plane, in order along an optical axis from an object side to an image side. The number of the lenses having refractive power in the optical image capturing system is seven. Each of at least three lenses among the first to the seventh lenses has at least an inflection point. The first lens has positive refractive power, and the second lens has refractive power. The third lens has refractive power. The fourth lens has refractive power. The fifth lens has refractive power. The sixth lens has refractive power. The seventh lens has refractive power. The optical image capturing system satisfies:

1.0≦f/HEP≦10.0; 0 deg<HAF≦150 deg; and 0.9≦2(ARE/HEP)≦1.5;

where f1, f2, f3, f4, f5, f6, and f7 are respectively the focal lengths of the first lens to the seventh lens; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HOS is a distance in parallel with the optical axis between an object-side surface, which face the object side, of the first lens and the image plane; InTL is a distance between the object-side surface of the first lens and the image-side surface of the seventh lens on the optical axis; HAF is a half of the maximum field angle; ARE is a profile curve length measured from a start point where the optical axis of the belonging optical image capturing system passes through the surface of the lens, along a surface profile of the lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis.

For any surface of any lens, the profile curve length within the effective half diameter affects the ability of the surface to correct aberration and differences between optical paths of light in different fields of view. With longer profile curve length, the ability to correct aberration is better. However, the difficulty of manufacturing increases as well. Therefore, the profile curve length within the effective half diameter of any surface of any lens has to be controlled. The ratio between the profile curve length (ARS) within the effective half diameter of one surface and the thickness (TP) of the lens, which the surface belonged to, on the optical axis (i.e., ARS/TP) has to be particularly controlled. For example, the profile curve length of the maximum effective half diameter of the object-side surface of the first lens is denoted by ARS11, the thickness of the first lens on the optical axis is TP1, and the ratio between these two parameters is ARS11/TP1; the profile curve length of the maximum effective half diameter of the image-side surface of the first lens is denoted by ARS12, and the ratio between ARS12 and TP1 is ARS12/TP1. The profile curve length of the maximum effective half diameter of the object-side surface of the second lens is denoted by ARS21, the thickness of the second lens on the optical axis is TP2, and the ratio between these two parameters is ARS21/TP2; the profile curve length of the maximum effective half diameter of the image-side surface of the second lens is denoted by ARS22, and the ratio between ARS22 and TP2 is ARS22/TP2. For any surface of other lenses in the optical image capturing system, the ratio between the profile curve length of the maximum effective half diameter thereof and the thickness of the lens which the surface belonged to is denoted in the same manner.

For any surface of any lens, the profile curve length within a half of the entrance pupil diameter (HEP) affects the ability of the surface to correct aberration and differences between optical paths of light in different fields of view. With longer profile curve length, the ability to correct aberration is better. However, the difficulty of manufacturing increases as well. Therefore, the profile curve length within a half of the entrance pupil diameter (HEP) of any surface of any lens has to be controlled. The ratio between the profile curve length (ARE) within a half of the entrance pupil diameter (HEP) of one surface and the thickness (TP) of the lens, which the surface belonged to, on the optical axis (i.e., ARE/TP) has to be particularly controlled. For example, the profile curve length of a half of the entrance pupil diameter (HEP) of the object-side surface of the first lens is denoted by ARE11, the thickness of the first lens on the optical axis is TP1, and the ratio between these two parameters is ARE11/TP1; the profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the first lens is denoted by ARE12, and the ratio between ARE12 and TP1 is ARE12/TP1. The profile curve length of a half of the entrance pupil diameter (HEP) of the object-side surface of the second lens is denoted by ARE21, the thickness of the second lens on the optical axis is TP2, and the ratio between these two parameters is ARE21/TP2; the profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the second lens is denoted by ARE22, and the ratio between ARE22 and TP2 is ARE22/TP2. For any surface of other lenses in the optical image capturing system, the ratio between the profile curve length of a half of the entrance pupil diameter (HEP) thereof and the thickness of the lens which the surface belonged to is denoted in the same manner.

In an embodiment, a height of the optical image capturing system (HOS) can be reduced if |f1|>|f7|.

In an embodiment, when |f2|+|f3|+|f4|+|f5|+|f6| and |f1|+|f7| of the lenses satisfy the aforementioned conditions, at least one lens among the second to the sixth lenses could have weak positive refractive power or weak negative refractive power. Herein the weak refractive power means the absolute value of the focal length of one specific lens is greater than 10. When at least one lens among the second to the sixth lenses has weak positive refractive power, it may share the positive refractive power of the first lens, and on the contrary, when at least one lens among the second to the sixth lenses has weak negative refractive power, it may fine turn and correct the aberration of the system.

In an embodiment, the seventh lens could have negative refractive power, and an image-side surface thereof is concave, it may reduce back focal length and size. Besides, the seventh lens can have at least an inflection point on at least a surface thereof, which may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWINGS

The present invention will be best understood by referring to the following detailed description of some illustrative embodiments in conjunction with the accompanying drawings, in which

FIG. 1A is a schematic diagram of a first embodiment of the present invention;

FIG. 1B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the first embodiment of the present application;

FIG. 1C shows a tangential fan and a sagittal fan of the optical image capturing system of the first embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 2A is a schematic diagram of a second embodiment of the present invention;

FIG. 2B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the second embodiment of the present application;

FIG. 2C shows a tangential fan and a sagittal fan of the optical image capturing system of the second embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 3A is a schematic diagram of a third embodiment of the present invention;

FIG. 3B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the third embodiment of the present application;

FIG. 3C shows a tangential fan and a sagittal fan of the optical image capturing system of the third embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 4A is a schematic diagram of a fourth embodiment of the present invention;

FIG. 4B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the fourth embodiment of the present application;

FIG. 4C shows a tangential fan and a sagittal fan of the optical image capturing system of the fourth embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 5A is a schematic diagram of a fifth embodiment of the present invention;

FIG. 5B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the fifth embodiment of the present application;

FIG. 5C shows a tangential fan and a sagittal fan of the optical image capturing system of the fifth embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 6A is a schematic diagram of a sixth embodiment of the present invention;

FIG. 6B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the sixth embodiment of the present application;

FIG. 6C shows a tangential fan and a sagittal fan of the optical image capturing system of the sixth embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 7A is a schematic diagram of a seventh embodiment of the present invention;

FIG. 7B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the seventh embodiment of the present application;

FIG. 7C shows a tangential fan and a sagittal fan of the optical image capturing system of the seventh embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 8A is a schematic diagram of a eighth embodiment of the present invention;

FIG. 8B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the eighth embodiment of the present application; and

FIG. 8C shows a tangential fan and a sagittal fan of the optical image capturing system of the eighth embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture.

DETAILED DESCRIPTION OF THE INVENTION

An optical image capturing system of the present invention includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and an image plane from an object side to an image side. The optical image capturing system further is provided with an image sensor at an image plane, wherein the image heights of the following embodiments are all around 3.91 mm.

The optical image capturing system can work in three wavelengths, including 486.1 nm, 587.5 nm, and 656.2 nm, wherein 587.5 nm is the main reference wavelength and is the reference wavelength for obtaining the technical characters. The optical image capturing system can also work in five wavelengths, including 470 nm, 510 nm, 555 nm, 610 nm, and 650 nm wherein 555 nm is the main reference wavelength, and is the reference wavelength for obtaining the technical characters.

The optical image capturing system of the present invention satisfies 0.5≦ΣPPR/|ΣNPR|≦15, and a preferable range is 1≦ΣPPR/|ΣNPR|≦3.0, where PPR is a ratio of the focal length f of the optical image capturing system to a focal length fp of each of lenses with positive refractive power; NPR is a ratio of the focal length f of the optical image capturing system to a focal length fn of each of lenses with negative refractive power; ΣPPR is a sum of the PPRs of each positive lens; and ΣNPR is a sum of the NPRs of each negative lens. It is helpful for control of an entire refractive power and an entire length of the optical image capturing system.

The image sensor is provided on the image plane. The optical image capturing system of the present invention satisfies HOS/HOI≦10; and 0.5≦HOS/f≦10, and a preferable range is 1≦HOS/HOI≦5; and 1≦HOS/f≦7, where HOI is a half of a diagonal of an effective sensing area of the image sensor, i.e., the maximum image height, and HOS is a height of the optical image capturing system, i.e. a distance on the optical axis between the object-side surface of the first lens and the image plane. It is helpful for reduction of the size of the system for used in compact cameras.

The optical image capturing system of the present invention further is provided with an aperture to increase image quality.

In the optical image capturing system of the present invention, the aperture could be a front aperture or a middle aperture, wherein the front aperture is provided between the object and the first lens, and the middle is provided between the first lens and the image plane. The front aperture provides a long distance between an exit pupil of the system and the image plane, which allows more elements to be installed. The middle could enlarge a view angle of view of the system and increase the efficiency of the image sensor. The optical image capturing system satisfies 0.2≦InS/HOS≦1.1, where InS is a distance between the aperture and the image-side surface of the sixth lens. It is helpful for size reduction and wide angle.

The optical image capturing system of the present invention satisfies 0.1≦ΣTP/InTL≦0.9, where InTL is a distance between the object-side surface of the first lens and the image-side surface of the seventh lens, and ΣTP is a sum of central thicknesses of the lenses on the optical axis. It is helpful for the contrast of image and yield rate of manufacture and provides a suitable back focal length for installation of other elements.

The optical image capturing system of the present invention satisfies 0.001≦|R1/R2|≦20, and a preferable range is 0.01≦|R1/R2|≦10, where R1 is a radius of curvature of the object-side surface of the first lens, and R2 is a radius of curvature of the image-side surface of the first lens. It provides the first lens with a suitable positive refractive power to reduce the increase rate of the spherical aberration.

The optical image capturing system of the present invention satisfies −7<(R13−R14)/(R13+R14)<50, where R13 is a radius of curvature of the object-side surface of the seventh lens, and R14 is a radius of curvature of the image-side surface of the seventh lens. It may modify the astigmatic field curvature.

The optical image capturing system of the present invention satisfies IN12/f≦3.0, where IN12 is a distance on the optical axis between the first lens and the second lens. It may correct chromatic aberration and improve the performance.

The optical image capturing system of the present invention satisfies IN67/f≦0.8, where IN67 is a distance on the optical axis between the sixth lens and the seventh lens. It may correct chromatic aberration and improve the performance.

The optical image capturing system of the present invention satisfies 0.1≦(TP1+IN12)/TP2≦10, where TP1 is a central thickness of the first lens on the optical axis, and TP2 is a central thickness of the second lens on the optical axis. It may control the sensitivity of manufacture of the system and improve the performance.

The optical image capturing system of the present invention satisfies 0.1≦(TP7+IN67)/TP6≦10, where TP6 is a central thickness of the sixth lens on the optical axis, TP7 is a central thickness of the seventh lens on the optical axis, and IN67 is a distance between the sixth lens and the seventh lens. It may control the sensitivity of manufacture of the system and improve the performance.

The optical image capturing system of the present invention satisfies 0.1≦TP4/(IN34+TP4+IN45)<1, where TP3 is a central thickness of the third lens on the optical axis, TP4 is a central thickness of the fourth lens on the optical axis, TP5 is a central thickness of the fifth lens on the optical axis, IN34 is a distance on the optical axis between the third lens and the fourth lens, IN45 is a distance on the optical axis between the fourth lens and the fifth lens, and InTL is a distance between the object-side surface of the first lens and the image-side surface of the seventh lens. It may fine tune and correct the aberration of the incident rays layer by layer, and reduce the height of the system.

The optical image capturing system satisfies 0 mm≦HVT71≦3 mm; 0 mm<HVT72≦6 mm; 0≦HVT71/HVT72; 0 mm≦|SGC71|≦0.5 mm; 0 mm≦|SGC72|≦2 mm; and 0<|SGC72|/(|SGC72|+TP7)≦0.9, where HVT71 a distance perpendicular to the optical axis between the critical point C71 on the object-side surface of the seventh lens and the optical axis; HVT72 a distance perpendicular to the optical axis between the critical point C72 on the image-side surface of the seventh lens and the optical axis; SGC71 is a distance in parallel with the optical axis between an point on the object-side surface of the seventh lens where the optical axis passes through and the critical point C71; SGC72 is a distance in parallel with the optical axis between an point on the image-side surface of the seventh lens where the optical axis passes through and the critical point C72 . It is helpful to correct the off-axis view field aberration.

The optical image capturing system satisfies 0.2≦HVT72/HOI≦0.9, and preferably satisfies 0.3≦HVT72/HOI≦0.8. It may help to correct the peripheral aberration.

The optical image capturing system satisfies 0≦HVT72/HOS≦0.5, and preferably satisfies 0.2≦HVT72/HOS≦0.45. It may help to correct the peripheral aberration.

The optical image capturing system of the present invention satisfies 0<SGI711/(SGI711+TP7)≦0.9; 0<SGI721/(SGI721+TP7)≦0.9, and it is preferable to satisfy 0.1≦SGI711/(SGI711+TP7)≦0.6; 0.1≦SGI721/(SGI721+TP7)≦0.6, where SGI711 is a displacement in parallel with the optical axis, from a point on the object-side surface of the seventh lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the closest to the optical axis, and SGI721 is a displacement in parallel with the optical axis, from a point on the image-side surface of the seventh lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the closest to the optical axis.

The optical image capturing system of the present invention satisfies 0<SGI712/(SGI712+TP7)≦0.9; 0<SGI722/(SGI722+TP7)≦0.9, and it is preferable to satisfy 0.1≦SGI712/(SGI712+TP7)≦0.6; 0.1≦SGI722/(SGI722+TP7)≦0.6, where SGI712 is a displacement in parallel with the optical axis, from a point on the object-side surface of the seventh lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the second closest to the optical axis, and SGI722 is a displacement in parallel with the optical axis, from a point on the image-side surface of the seventh lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the second closest to the optical axis.

The optical image capturing system of the present invention satisfies 0.001 mm≦|HIF711|≦5 mm; 0.001 mm≦|HIF721|≦5 mm, and it is preferable to satisfy 0.1 mm≦|HIF711|≦3.5 mm; 1.5 mm≦|HIF721|≦3.5 mm, where HIF711 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the closest to the optical axis, and the optical axis; HIF721 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the closest to the optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies 0.001 mm≦|HIF712|≦5 mm; 0.001 mm≦|HIF722|≦5 mm, and it is preferable to satisfy 0.1 mm≦|HIF722|≦3.5 mm; 0.1 mm≦|HIF712|≦3.5 mm, where HIF712 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the second closest to the optical axis, and the optical axis; HIF722 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the second closest to the optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies 0.001 mm≦|HIF713|≦5 mm; 0.001 mm≦|HIF723|≦5 mm, and it is preferable to satisfy 0.1 mm≦|HIF723|≦3.5 mm; 0.1 mm≦|HIF713|≦3.5 mm, where HIF713 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the third closest to the optical axis, and the optical axis; HIF723 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the third closest to the optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies 0.001 mm≦|HIF714|≦5 mm; 0.001 mm≦|HIF724|≦5 mm, and it is preferable to satisfy 0.1 mm≦|HIF724|≦3.5 mm; 0.1 mm≦|HIF714|≦3.5 mm, where HIF714 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the fourth closest to the optical axis, and the optical axis; HIF724 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the fourth closest to the optical axis, and the optical axis.

In an embodiment, the lenses of high Abbe number and the lenses of low Abbe number are arranged in an interlaced arrangement that could be helpful for correction of aberration of the system.

An equation of aspheric surface is

z=ch ₂/[1+[1(k+1)c ² h ²]^(0.5) ]+A4h ⁴ +A6h ⁶ +A8h ⁸ +A10h ¹⁰ +A12h ¹² +A14h ¹⁴ +A16h ¹⁶ +A18h ¹⁸ +A20h ²⁰+   (1)

where z is a depression of the aspheric surface; k is conic constant; c is reciprocal of the radius of curvature; and A4, A6, A8, A10, Al2, A14, A16, A18, and A20 are high-order aspheric coefficients.

In the optical image capturing system, the lenses could be made of plastic or glass. The plastic lenses may reduce the weight and lower the cost of the system, and the glass lenses may control the thermal effect and enlarge the space for arrangement of the refractive power of the system. In addition, the opposite surfaces (object-side surface and image-side surface) of the first to the seventh lenses could be aspheric that can obtain more control parameters to reduce aberration. The number of aspheric glass lenses could be less than the conventional spherical glass lenses, which is helpful for reduction of the height of the system.

When the lens has a convex surface, which means that the surface is convex around a position, through which the optical axis passes, and when the lens has a concave surface, which means that the surface is concave around a position, through which the optical axis passes.

The optical image capturing system of the present invention could be applied in a dynamic focusing optical system. It is superior in the correction of aberration and high imaging quality so that it could be allied in lots of fields.

The optical image capturing system of the present invention could further include a driving module to meet different demands, wherein the driving module can be coupled with the lenses to move the lenses. The driving module can be a voice coil motor (VCM), which is used to move the lens for focusing, or can be an optical image stabilization (OIS) component, which is used to lower the possibility of having the problem of image blurring which is caused by subtle movements of the lens while shooting.

To meet different requirements, at least one lens among the first lens to the seventh lens of the optical image capturing system of the present invention can be a light filter, which filters out light of wavelength shorter than 500 nm. Such effect can be achieved by coating on at least one surface of the lens, or by using materials capable of filtering out short waves to make the lens.

We provide several embodiments in conjunction with the accompanying drawings for the best understanding, which are:

First Embodiment

As shown in FIG. 1A and FIG. 1B, an optical image capturing system 10 of the first embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 110, an aperture 100, a second lens 120, a third lens 130, a fourth lens 140, a fifth lens 150, a sixth lens 160, a seventh lens 170, an infrared rays filter 180, an image plane 190, and an image sensor 192. FIG. 1C shows a tangential fan and a sagittal fan of the optical image capturing system 10 of the first embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of the aperture 100.

The first lens 110 has negative refractive power and is made of plastic. An object-side surface 112 thereof, which faces the object side, is a concave aspheric surface, and an image-side surface 114 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 112 has an inflection point, and the image-side surface 114 has two inflection points. A profile curve length of the maximum effective half diameter of an object-side surface of the first lens 110 is denoted by ARS11, and a profile curve length of the maximum effective half diameter of the image-side surface of the first lens 110 is denoted by ARS12. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the first lens 110 is denoted by ARE11, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the first lens 110 is denoted by ARE12. A thickness of the first lens 110 on the optical axis is TP1.

The first lens 110 satisfies SGI111=−0.1110 mm; SGI121=2.7120 mm; TP1=2.2761 mm; |SGI111|/(|SGI111|+TP1)=0.0465; |SGI121|/(|SGI121|+TP1)=0.5437, where a displacement in parallel with the optical axis from a point on the object-side surface of the first lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the closest to the optical axis is denoted by SGI111, and a displacement in parallel with the optical axis from a point on the image-side surface of the first lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the closest to the optical axis is denoted by SGI121.

The first lens 110 satisfies SGI112=0 mm; SGI122=4.2315 mm; |SGI112|/(|SGI112|+TP1)=0; |SGI122|/(|SGI122|+TP1)=0.6502, where a displacement in parallel with the optical axis from a point on the object-side surface of the first lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the second closest to the optical axis is denoted by SGI112, and a displacement in parallel with the optical axis from a point on the image-side surface of the first lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the second closest to the optical axis is denoted by SGI122.

The first lens 110 satisfies HIF111=12.8432 mm; HIF111/HOI=1.7127; HIF121=7.1744 mm; HIF121/HOI=0.9567, where a displacement perpendicular to the optical axis from a point on the object-side surface of the first lens, through which the optical axis passes, to the inflection point, which is the closest to the optical axis is denoted by HIF111, and a displacement perpendicular to the optical axis from a point on the image-side surface of the first lens, through which the optical axis passes, to the inflection point, which is the closest to the optical axis is denoted by HIF121.

The first lens 110 satisfies HIF112=0 mm; HIF112/HOI=0; HIF122=9.8592 mm; HIF122/HOI=1.3147, where a displacement perpendicular to the optical axis from a point on the object-side surface of the first lens, through which the optical axis passes, to the inflection point, which is the second closest to the optical axis is denoted by HIF112, and a displacement perpendicular to the optical axis from a point on the image-side surface of the first lens, through which the optical axis passes, to the inflection point, which is the second closest to the optical axis is denoted by HIF122.

The second lens 120 has positive refractive power and is made of plastic. An object-side surface 122 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 124 thereof, which faces the image side, is a concave aspheric surface. A profile curve length of the maximum effective half diameter of an object-side surface of the second lens 120 is denoted by ARS21, and a profile curve length of the maximum effective half diameter of the image-side surface of the second lens 120 is denoted by ARS22. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the second lens 120 is denoted by ARE21, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the second lens 120 is denoted by ARE22. A thickness of the second lens 120 on the optical axis is TP2.

For the second lens 120, a displacement in parallel with the optical axis from a point on the object-side surface of the second lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the closest to the optical axis is denoted by SGI211, and a displacement in parallel with the optical axis from a point on the image-side surface of the second lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the closest to the optical axis is denoted by SGI221.

For the second lens, a displacement perpendicular to the optical axis from a point on the object-side surface of the second lens, through which the optical axis passes, to the inflection point, which is the closest to the optical axis is denoted by HIF211, and a displacement perpendicular to the optical axis from a point on the image-side surface of the second lens, through which the optical axis passes, to the inflection point, which is the closest to the optical axis is denoted by HIF221.

The third lens 130 has negative refractive power and is made of plastic. An object-side surface 132, which faces the object side, is a convex aspheric surface, and an image-side surface 134, which faces the image side, is a concave aspheric surface. A profile curve length of the maximum effective half diameter of an object-side surface of the third lens 130 is denoted by ARS31, and a profile curve length of the maximum effective half diameter of the image-side surface of the third lens 130 is denoted by ARS32. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the third lens 130 is denoted by ARE31, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the third lens 130 is denoted by ARE32. A thickness of the third lens 130 on the optical axis is TP3.

For the third lens 130, SGI311 is a displacement in parallel with the optical axis, from a point on the object-side surface of the third lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the closest to the optical axis, and SGI321 is a displacement in parallel with the optical axis, from a point on the image-side surface of the third lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the closest to the optical axis.

For the third lens 130, SGI312 is a displacement in parallel with the optical axis, from a point on the object-side surface of the third lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the second closest to the optical axis, and SGI322 is a displacement in parallel with the optical axis, from a point on the image-side surface of the third lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the second closest to the optical axis.

For the third lens 130, HIF311 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the third lens, which is the closest to the optical axis, and the optical axis; HIF321 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the third lens, which is the closest to the optical axis, and the optical axis.

For the third lens 130, HIF312 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the third lens, which is the second closest to the optical axis, and the optical axis; HIF322 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the third lens, which is the second closest to the optical axis, and the optical axis.

The fourth lens 140 has positive refractive power and is made of plastic. An object-side surface 142, which faces the object side, is a convex aspheric surface, and an image-side surface 144, which faces the image side, is a convex aspheric surface. The object-side surface 142 has an inflection point. A profile curve length of the maximum effective half diameter of an object-side surface of the fourth lens 140 is denoted by ARS41, and a profile curve length of the maximum effective half diameter of the image-side surface of the fourth lens 140 is denoted by ARS42. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the fourth lens 140 is denoted by ARE41, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the fourth lens 140 is denoted by ARE42. A thickness of the fourth lens 140 on the optical axis is TP4.

The fourth lens 140 satisfies SGI411=0.0018 mm; |SGI411|/(|SGI411|+TP4)=0.0009, where SGI411 is a displacement in parallel with the optical axis, from a point on the object-side surface of the fourth lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the closest to the optical axis, and SGI421 is a displacement in parallel with the optical axis, from a point on the image-side surface of the fourth lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the closest to the optical axis.

For the fourth lens 140, SGI412 is a displacement in parallel with the optical axis, from a point on the object-side surface of the fourth lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the second closest to the optical axis, and SGI422 is a displacement in parallel with the optical axis, from a point on the image-side surface of the fourth lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the second closest to the optical axis.

The fourth lens 140 further satisfies HIF411=0.7191 mm; HIF411/HIF411/HOI=0.0959, where HIF411 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens, which is the closest to the optical axis, and the optical axis; HIF421 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the fourth lens, which is the closest to the optical axis, and the optical axis.

For the fourth lens 140, HIF412 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens, which is the second closest to the optical axis, and the optical axis; HIF422 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the fourth lens, which is the second closest to the optical axis, and the optical axis.

The fifth lens 150 has positive refractive power and is made of plastic. An object-side surface 152, which faces the object side, is a concave aspheric surface, and an image-side surface 154, which faces the image side, is a convex aspheric surface. The object-side surface 152 and the image-side surface 154 both have an inflection point. A profile curve length of the maximum effective half diameter of an object-side surface of the fifth lens 150 is denoted by ARS51, and a profile curve length of the maximum effective half diameter of the image-side surface of the fifth lens 150 is denoted by ARS52. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the fifth lens 150 is denoted by ARE51, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the fifth lens 150 is denoted by ARE52. A thickness of the fifth lens 150 on the optical axis is TP5.

The fifth lens 150 satisfies SGI511=−0.1246 mm; SGI521=−2.1477 mm; |SGI511|/(|SGI511|+TP5)=0.0284; |SGI521|/(|SGI521|+TP5)=0.3346, where SGI511 is a displacement in parallel with the optical axis, from a point on the object-side surface of the fifth lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the closest to the optical axis, and SGI521 is a displacement in parallel with the optical axis, from a point on the image-side surface of the fifth lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the closest to the optical axis.

For the fifth lens 150, SGI512 is a displacement in parallel with the optical axis, from a point on the object-side surface of the fifth lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the second closest to the optical axis, and SGI522 is a displacement in parallel with the optical axis, from a point on the image-side surface of the fifth lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the second closest to the optical axis.

The fifth lens 150 further satisfies HIF511=3.8179 mm; HIF521=4.5480 mm; HIF511/HOI=0.5091; HIF521/HOI=0.6065, where HIF511 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the fifth lens, which is the closest to the optical axis, and the optical axis; HIF521 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the fifth lens, which is the closest to the optical axis, and the optical axis.

For the fifth lens 150, HIF512 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the fifth lens, which is the second closest to the optical axis, and the optical axis; HIF522 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the fifth lens, which is the second closest to the optical axis, and the optical axis.

The sixth lens 160 has negative refractive power and is made of plastic. An object-side surface 162, which faces the object side, is a convex surface, and an image-side surface 164, which faces the image side, is a concave surface. The object-side surface 162 and the image-side surface 164 both have an inflection point. Whereby, incident angle of each field of view for the sixth lens can be effectively adjusted to improve aberration. A profile curve length of the maximum effective half diameter of an object-side surface of the sixth lens 160 is denoted by ARS61, and a profile curve length of the maximum effective half diameter of the image-side surface of the sixth lens 160 is denoted by ARS62. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the sixth lens 160 is denoted by ARE61, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the sixth lens 160 is denoted by ARE62. A thickness of the sixth lens 160 on the optical axis is TP6.

The sixth lens 160 satisfies SGI611=0.3208 mm; SGI621=0.5937 mm; |SGI611|/(|SGI611|+TP6)=0.5167; |SGI621|/(|SGI621|+TP6)=0.6643, where SGI611 is a displacement in parallel with the optical axis, from a point on the object-side surface of the sixth lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the closest to the optical axis, and SGI621 is a displacement in parallel with the optical axis, from a point on the image-side surface of the sixth lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the closest to the optical axis.

The sixth lens 160 further satisfies HIF611=1.9655 mm; HIF621=2.0041 mm; HIF611/HOI=0.2621; HIF621/HOI=0.2672, where HIF611 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the sixth lens, which is the closest to the optical axis, and the optical axis; HIF621 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the sixth lens, which is the closest to the optical axis, and the optical axis.

The seventh lens 170 has positive refractive power and is made of plastic. An object-side surface 172, which faces the object side, is a convex surface, and an image-side surface 174, which faces the image side, is a concave surface. Whereby, it is helpful to shorten the focal length behind the seventh lens for miniaturization. The object-side surface 172 and the image-side surface 174 both have an inflection point. A profile curve length of the maximum effective half diameter of an object-side surface of the seventh lens 170 is denoted by ARS71, and a profile curve length of the maximum effective half diameter of the image-side surface of the seventh lens 170 is denoted by ARS72. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the seventh lens 170 is denoted by ARE71, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the seventh lens 170 is denoted by ARE72. A thickness of the seventh lens 170 on the optical axis is TP7.

The seventh lens 170 satisfies SGI711=0.5212 mm; SGI721=0.5668 mm; |SGI711|/(|SGI711|+TP7)=0.3179; |SGI721|/(|SGI721|+TP7)=0.3364, where SGI711 is a displacement in parallel with the optical axis, from a point on the object-side surface of the seventh lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the closest to the optical axis, and SGI721 is a displacement in parallel with the optical axis, from a point on the image-side surface of the seventh lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the closest to the optical axis.

The seventh lens 170 further satisfies HIF711=1.6707 mm; HIF721=1.8616 mm; HIF711/HOI=0.2228; HIF721/HOI=0.2482, where HIF711 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the closest to the optical axis, and the optical axis; HIF721 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the closest to the optical axis, and the optical axis.

The features related to the inflection points in the present embodiment described below are obtained with the main reference wavelength 555 nm.

The infrared rays filter 180 is made of glass and between the seventh lens 170 and the image plane 190. The infrared rays filter 180 gives no contribution to the focal length of the system.

The optical image capturing system 10 of the first embodiment has the following parameters, which are f=4.3019 mm; f/HEP=1.2; HAF=59.9968; and tan(HAF)=1.7318, where f is a focal length of the system; HAF is a half of the maximum field angle; and HEP is an entrance pupil diameter.

The parameters of the lenses of the first embodiment are f1=−14.5286 mm; |f/f1|=0.2961; f7=8.2933; |f1|>f7; and |f1/f7|=1.7519, where f1 is a focal length of the first lens 110; and f7 is a focal length of the seventh lens 170.

The first embodiment further satisfies |f2|+|f3|+|f4|+|f5|+‥f6|=144.7494; |f1|+|f7|=22.8219 and |f2|+|f3|+|f4|+|f5|+|f6|>|f1|+|f7|, where f2 is a focal length of the second lens 120, f3 is a focal length of the third lens 130, f4 is a focal length of the fourth lens 140, f5 is a focal length of the fifth lens 150, f6 is a focal length of the sixth lens 160, and f7 is a focal length of the seventh lens 170.

The optical image capturing system 10 of the first embodiment further satisfies ΣPPR=f/f2+f/f4+f/f5+f/f7=1.7384; ΣNPR=f/f1+f/f3+f/f6=−0.9999; ΣPPR/|ΣNPR|=1.7386; |f/f2|=0.1774; |f/f3|=0.0443; |f/f4|=0.4411; |f/f5|=0.6012; |f/f6|=0.6595; |f/f7|=0.5187, where PPR is a ratio of a focal length f of the optical image capturing system to a focal length fp of each of the lenses with positive refractive power; and NPR is a ratio of a focal length f of the optical image capturing system to a focal length fn of each of lenses with negative refractive power.

The optical image capturing system 10 of the first embodiment further satisfies InTL+BFL=HOS; HOS=26.9789 mm; HOI=7.5 mm; HOS/HOI=3.5977; HOS/f=6.2715; InS=12.4615 mm; and InS/HOS=0.4619, where InTL is a distance between the object-side surface 112 of the first lens 110 and the image-side surface 174 of the seventh lens 170; HOS is a height of the image capturing system, i.e. a distance between the object-side surface 112 of the first lens 110 and the image plane 190; InS is a distance between the aperture 100 and the image plane 190; HOI is a half of a diagonal of an effective sensing area of the image sensor 192, i.e., the maximum image height; and BFL is a distance between the image-side surface 174 of the seventh lens 170 and the image plane 190.

The optical image capturing system 10 of the first embodiment further satisfies ΣTP=16.0446 mm; and ΣTP/InTL=0.6559, where ΣTP is a sum of the thicknesses of the lenses 110-170 with refractive power. It is helpful for the contrast of image and yield rate of manufacture and provides a suitable back focal length for installation of other elements.

The optical image capturing system 10 of the first embodiment further satisfies |R1/R2|=129.9952, where R1 is a radius of curvature of the object-side surface 112 of the first lens 110, and R2 is a radius of curvature of the image-side surface 114 of the first lens 110. It provides the first lens with a suitable positive refractive power to reduce the increase rate of the spherical aberration.

The optical image capturing system 10 of the first embodiment further satisfies (R13−R14)/(R13+R14)=−0.0806, where R13 is a radius of curvature of the object-side surface 172 of the seventh lens 170, and R14 is a radius of curvature of the image-side surface 174 of the seventh lens 170. It may modify the astigmatic field curvature.

The optical image capturing system 10 of the first embodiment further satisfies ΣPP=f2+f4+f5+f7=49.4535 mm; and f4/(f2+f4+f5+f7)=0.1972, where ΣPP is a sum of the focal lengths fp of each lens with positive refractive power. It is helpful to share the positive refractive power of the fourth lens 140 to other positive lenses to avoid the significant aberration caused by the incident rays.

The optical image capturing system 10 of the first embodiment further satisfies ΣNP=f1+f3+f6=−118.1178 mm; and f1/(f1+f3+f6)=0.1677, where ΣNP is a sum of the focal lengths fn of each lens with negative refractive power. It is helpful to share the negative refractive power of the first lens 110 to other negative lenses, which avoids the significant aberration caused by the incident rays.

The optical image capturing system 10 of the first embodiment further satisfies IN12=4.5524 mm; IN12/f =1.0582, where IN12 is a distance on the optical axis between the first lens 110 and the second lens 120. It may correct chromatic aberration and improve the performance.

The optical image capturing system 10 of the first embodiment further satisfies TP1=2.2761 mm; TP2=0.2398 mm; and (TP1+IN12)/TP2=1.3032, where TP1 is a central thickness of the first lens 110 on the optical axis, and TP2 is a central thickness of the second lens 120 on the optical axis. It may control the sensitivity of manufacture of the system and improve the performance.

The optical image capturing system 10 of the first embodiment further satisfies TP6=0.3000 mm; TP7=1.1182 mm; and (TP7+IN67)/TP6=4.4322, where TP6 is a central thickness of the sixth lens 160 on the optical axis, TP7 is a central thickness of the seventh lens 170 on the optical axis, and IN67 is a distance on the optical axis between the sixth lens 160 and the seventh lens 170. It may control the sensitivity of manufacture of the system and lower the total height of the system.

The optical image capturing system 10 of the first embodiment further satisfies TP3=0.8369 mm; TP4=2.0022 mm; TP5=4.2706 mm; IN34=1.9268 mm; IN45=1.5153 mm; and TP4/(IN34+TP4+IN45)=0.3678, where TP3 is a central thickness of the third lens 130 on the optical axis, TP4 is a central thickness of the fourth lens 140 on the optical axis, TP5 is a central thickness of the fifth lens 150 on the optical axis, IN34 is a distance on the optical axis between the third lens 130 and the fourth lens 140, and IN45 is a distance on the optical axis between the fourth lens 140 and the fifth lens 150. It may control the sensitivity of manufacture of the system and lower the total height of the system.

The optical image capturing system 10 of the first embodiment further satisfies InRS61=−0.7823 mm; InRS62=−0.2166 mm; and |InRS62|/TP6 =0.722, where InRS61 is a displacement in parallel with the optical axis from a point on the object-side surface 162 of the sixth lens 160, through which the optical axis passes, to a point at the maximum effective semi diameter of the object-side surface 162 of the sixth lens; InRS62 is a displacement in parallel with the optical axis from a point on the image-side surface 164 of the sixth lens 160, through which the optical axis passes, to a point at the maximum effective semi diameter of the image-side surface 164 of the sixth lens 160; and TP6 is a central thickness of the sixth lens 160 on the optical axis. It is helpful for manufacturing and shaping of the lenses and is helpful to reduce the size.

The optical image capturing system 10 of the first embodiment further satisfies HVT61=3.3498 mm; HVT62=3.9860 mm; and HVT61/HVT62=0.8404, where HVT61 a distance perpendicular to the optical axis between the critical point on the object-side surface 162 of the sixth lens 160 and the optical axis; and HVT62 a distance perpendicular to the optical axis between the critical point on the image-side surface 164 of the sixth lens 160 and the optical axis.

The optical image capturing system 10 of the first embodiment further satisfies InRS71=−0.2756 mm; InRS72=−0.0938 mm; and |InRS72|/TP7=0.0839, where InRS71 is a displacement in parallel with the optical axis from a point on the object-side surface 172 of the seventh lens 170, through which the optical axis passes, to a point at the maximum effective semi diameter of the object-side surface 172 of the seventh lens 170; InRS72 is a displacement in parallel with the optical axis from a point on the image-side surface 174 of the seventh lens 170, through which the optical axis passes, to a point at the maximum effective semi diameter of the image-side surface 174 of the seventh lens 170; and TP7 is a central thickness of the seventh lens 170 on the optical axis. It is helpful for manufacturing and shaping of the lenses and is helpful to reduce the size.

The optical image capturing system 10 of the first embodiment satisfies HVT71=3.6822 mm; HVT72=4.0606 mm; and HVT71/HVT72=0.9068, where HVT71 a distance perpendicular to the optical axis between the critical point on the object-side surface 172 of the seventh lens 170 and the optical axis; and HVT72 a distance perpendicular to the optical axis between the critical point on the image-side surface 174 of the seventh lens 170 and the optical axis.

The optical image capturing system 10 of the first embodiment satisfies HVT72/HOI=0.5414. It is helpful for correction of the aberration of the peripheral view field of the optical image capturing system.

The optical image capturing system 10 of the first embodiment satisfies HVT72/HOS=0.1505. It is helpful for correction of the aberration of the peripheral view field of the optical image capturing system.

The second lens 120, the third lens 130, and the seventh lens 170 have negative refractive power. The optical image capturing system 10 of the first embodiment further satisfies 1≦NA7/NA2, where NA2 is an Abbe number of the second lens 120; and NA7 is an Abbe number of the seventh lens 170. It may correct the aberration of the optical image capturing system.

The optical image capturing system 10 of the first embodiment further satisfies |TDT|=2.5678%; |ODT|=2.1302%, where TDT is TV distortion; and ODT is optical distortion.

For the fifth lens 150 of the optical image capturing system 10 in the first embodiment, a transverse aberration at 0.7 field of view in the positive direction of the tangential fan after the shortest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by PSTA, and is 0.00040 mm; a transverse aberration at 0.7 field of view in the positive direction of the tangential fan after the longest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by PLTA, and is −0.009 mm; a transverse aberration at 0.7 field of view in the negative direction of the tangential fan after the shortest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by NSTA, and is −0.002 mm; a transverse aberration at 0.7 field of view in the negative direction of the tangential fan after the longest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by NLTA, and is −0.016 mm; a transverse aberration at 0.7 field of view of the sagittal fan after the shortest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by SSTA, and is 0.018 mm; a transverse aberration at 0.7 field of view of the sagittal fan after the longest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by SLTA, and is 0.016 mm.

The parameters of the lenses of the first embodiment are listed in Table 1 and Table 2.

TABLE 1 f = 4.3019 mm; f/HEP = 1.2; HAF = 59.9968 deg Focal Radius of curvature Thickness Refractive Abbe length Surface (mm) (mm) Material index number (mm) 0 Object plane infinity 1 1^(st) lens −1079.499964 2.276 plastic 1.565 58.00 −14.53 2 8.304149657 4.552 3 2^(nd) lens 14.39130913 5.240 plastic 1.650 21.40 24.25 4 130.0869482 0.162 5 3^(rd) lens 8.167310118 0.837 plastic 1.650 21.40 −97.07 6 6.944477468 1.450 7 Aperture plane 0.477 8 4^(th) lens 121.5965254 2.002 plastic 1.565 58.00 9.75 9 −5.755749302 1.515 10 5^(th) lens −86.27705938 4.271 plastic 1.565 58.00 7.16 11 −3.942936258 0.050 12 6^(th) lens 4.867364751 0.300 plastic 1.650 21.40 −6.52 13 2.220604983 0.211 14 7^(th) lens 1.892510651 1.118 plastic 1.650 21.40 8.29 15 2.224128115 1.400 16 Infrared plane 0.200 BK_7 1.517 64.2 rays filter 17 plane 0.917 18 Image plane plane Reference wavelength (d-line): 555 nm.

TABLE 2 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k 2.500000E+01 −4.711931E−01 1.531617E+00 −1.153034E+01 −2.915013E+00 4.886991E+00 −3.459463E+01 A4 5.236918E−06 −2.117558E−04 7.146736E−05 4.353586E−04 5.793768E−04 −3.756697E−04 −1.292614E−03 A6 −3.014384E−08 −1.838670E−06 2.334364E−06 1.400287E−05 2.112652E−04 3.901218E−04 −1.602381E−05 A8 −2.487400E−10 9.605910E−09 −7.479362E−08 −1.688929E−07 −1.344586E−05 −4.925422E−05 −8.452359E−06 A10 1.170000E−12 −8.256000E−11 1.701570E−09 3.829807E−08 1.000482E−06 4.139741E−06 7.243999E−07 A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface 9 10 11 12 13 14 15 k −7.549291E+00 −5.000000E+01 −1.740728E+00 −4.709650E+00 −4.509781E+00 −3.427137E+00 −3.215123E+00 A4 −5.583548E−03 1.240671E−04 6.467538E−04 −1.872317E−03 −8.967310E−04 −3.189453E−03 −2.815022E−03 A6 1.947110E−04 −4.949077E−05 −4.981838E−05 −1.523141E−05 −2.688331E−05 −1.058126E−05 1.884580E−05 A8 −1.486947E−05 2.088854E−06 9.129031E−07 −2.169414E−06 −8.324958E−07 1.760103E−06 −1.017223E−08 A10 −6.501246E−08 −1.438383E−08 7.108550E−09 −2.308304E−08 −6.184250E−09 −4.730294E−08 3.660000E−12 A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

The figures related to the profile curve lengths obtained based on Table 1 and Table 2 are listed in the following table:

First embodiment (Reference wavelength: 555 nm) ARE − 2(ARE/HEP) ARE ½(HEP) ARE value ½(HEP) % TP ARE/TP (%) 11 1.792 1.792 −0.00044 99.98% 2.276 78.73% 12 1.792 1.806 0.01319 100.74% 2.276 79.33% 21 1.792 1.797 0.00437 100.24% 5.240 34.29% 22 1.792 1.792 −0.00032 99.98% 5.240 34.20% 31 1.792 1.808 0.01525 100.85% 0.837 216.01% 32 1.792 1.819 0.02705 101.51% 0.837 217.42% 41 1.792 1.792 −0.00041 99.98% 2.002 89.50% 42 1.792 1.825 0.03287 101.83% 2.002 91.16% 51 1.792 1.792 −0.00031 99.98% 4.271 41.96% 52 1.792 1.845 0.05305 102.96% 4.271 43.21% 61 1.792 1.818 0.02587 101.44% 0.300 606.10% 62 1.792 1.874 0.08157 104.55% 0.300 624.67% 71 1.792 1.898 0.10523 105.87% 1.118 169.71% 72 1.792 1.885 0.09273 105.17% 1.118 168.59% ARS EHD ARS value ARS − EHD (ARS/EHD) % TP ARS/TP (%) 11 15.095 15.096 0.001 100.01% 2.276 663.24% 12 10.315 11.377 1.062 110.29% 2.276 499.86% 21 7.531 8.696 1.166 115.48% 5.240 165.96% 22 4.759 4.881 0.122 102.56% 5.240 93.15% 31 3.632 4.013 0.382 110.51% 0.837 479.55% 32 2.815 3.159 0.344 112.23% 0.837 377.47% 41 2.967 2.971 0.004 100.13% 2.002 148.38% 42 3.402 3.828 0.426 112.53% 2.002 191.20% 51 4.519 4.523 0.004 100.10% 4.271 105.91% 52 5.016 5.722 0.706 114.08% 4.271 133.99% 61 5.019 5.823 0.805 116.04% 0.300 1941.14% 62 5.629 6.605 0.976 117.34% 0.300 2201.71% 71 5.634 6.503 0.869 115.43% 1.118 581.54% 72 6.488 7.152 0.664 110.24% 1.118 639.59%

The detail parameters of the first embodiment are listed in Table 1, in which the unit of the radius of curvature, thickness, and focal length are millimeter, and surface 0-10 indicates the surfaces of all elements in the system in sequence from the object side to the image side. Table 2 is the list of coefficients of the aspheric surfaces, in which A1-A20 indicate the coefficients of aspheric surfaces from the first order to the twentieth order of each aspheric surface. The following embodiments have the similar diagrams and tables, which are the same as those of the first embodiment, so we do not describe it again.

Second Embodiment

As shown in FIG. 2A and FIG. 2B, an optical image capturing system 20 of the second embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 210, an aperture 200, a second lens 220, a third lens 230, a fourth lens 240, a fifth lens 250, a sixth lens 260, a seven lens 270, an infrared rays filter 280, an image plane 290, and an image sensor 292. FIG. 2C is a transverse aberration diagram at 0.7 field of view of the second embodiment of the present application.

The first lens 210 has positive refractive power and is made of plastic. An object-side surface 212 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 214 thereof, which faces the image side, is a concave aspheric surface.

The second lens 220 has negative refractive power and is made of plastic. An object-side surface 222 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 224 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 222 has an inflection point, and the image-side surface 224 has two inflection points.

The third lens 230 has positive refractive power and is made of plastic. An object-side surface 232, which faces the object side, is a concave aspheric surface, and an image-side surface 234, which faces the image side, is a convex aspheric surface. The object-side surface 232 and the image-side surface 234 both have an inflection point.

The fourth lens 240 has positive refractive power and is made of plastic. An object-side surface 242, which faces the object side, is a convex aspheric surface, and an image-side surface 244, which faces the image side, is a convex aspheric surface. The object-side surface 242 and the image-side surface 244 both have an inflection point.

The fifth lens 250 has negative refractive power and is made of plastic. An object-side surface 252, which faces the object side, is a concave aspheric surface, and an image-side surface 254, which faces the image side, is a convex aspheric surface. The image-side surface 254 has an inflection point.

The sixth lens 260 has positive refractive power and is made of plastic. An object-side surface 262, which faces the object side, is a convex aspheric surface, and an image-side surface 264, which faces the image side, is a convex aspheric surface. The object-side surface 262 has an inflection point, and the image-side surface 264 has two inflection points. Whereby, incident angle of each field of view for the sixth lens can be effectively adjusted to improve aberration.

The seventh lens 270 has negative refractive power and is made of plastic. An object-side surface 272, which faces the object side, is a concave surface, and an image-side surface 274, which faces the image side, is a concave surface. It may help to shorten the back focal length to keep small in size. In addition, for the seventh lens 270, the object-side surface 272 has two inflection points, and the image-side surface 274 has an inflection point, which may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 280 is made of glass and between the seventh lens 270 and the image plane 290. The infrared rays filter 280 gives no contribution to the focal length of the system.

In the second embodiment, the optical image capturing system of the second embodiment further satisfies ΣPP=112.6399 mm; and f1/ΣPP=0.0907, where ΣPP is a sum of the focal lengths of each positive lens. It is helpful to share the positive refractive power of one single lens to other positive lenses to avoid the significant aberration caused by the incident rays.

The optical image capturing system of the second embodiment further satisfies ΣNP=−58.9049 mm; and f7/ΣNP =0.1182, where ΣNP is a sum of the focal lengths of each negative lens. It is helpful to share the negative refractive power of one single lens to other negative lenses.

The parameters of the lenses of the second embodiment are listed in Table 3 and Table 4.

TABLE 3 f = 7.3981 mm; f/HEP = 1.4; HAF = 37.5 deg Focal Radius of curvature Thickness Refractive Abbe length Surface (mm) (mm) Material index number (mm) 0 Object plane infinity 1 1^(st) lens 4.540107024 1.702 plastic 1.565 58.00 10.221 2 18.14724612 0.208 3 Aperture plane 0.165 4 2^(nd) lens 3.639282865 0.300 plastic 1.650 21.40 −28.437 5 2.945398119 0.519 6 3^(rd) lens −32.97337991 1.172 plastic 1.565 58.00 14.202 7 −6.553207522 0.244 8 4^(th) lens 11.83806932 0.478 plastic 1.607 26.60 81.729 9 15.27791187 1.363 10 5^(th) lens −1.539619547 0.662 plastic 1.650 21.40 −23.505 11 −2.001908277 0.050 12 6^(th) lens 4.851764306 1.300 plastic 1.607 26.60 6.488 13 −19.48629895 0.768 14 7^(th) lens −7.112479218 0.581 plastic 1.650 21.40 −6.963 15 13.14911542 1.000 16 Infrared plane 0.300 BK_7 1.517 64.2 rays filter 17 plane 0.044 18 Image plane 0.095 plane Reference wavelength (d-line): 555 nm.

TABLE 4 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k −4.875568E+00 −5.000000E+01 −1.676073E+01 −4.680304E+00 5.000000E+01 3.721744E+00 −5.000000E+01 A4 7.344150E−03 −3.973450E−03 2.662221E−03 −1.308314E−02 4.964298E−05 −8.260152E−03 −1.095602E−02 A6 −7.459683E−04 1.760892E−03 −1.131725E−02 1.646226E−03 5.872398E−04 7.786565E−05 −3.039081E−03 A8 2.242006E−04 −1.686811E−04 5.584613E−03 −8.461823E−06 −2.155411E−04 6.502447E−04 1.162066E−03 A10 −4.894969E−05 −6.697240E−05 −1.702728E−03 −8.784909E−05 5.116732E−05 −2.619295E−04 −3.599534E−04 A12 6.784149E−06 2.498565E−05 3.110902E−04 1.922030E−05 −1.669358E−05 4.823445E−05 5.939494E−05 A14 −4.968050E−07 −3.231451E−06 −3.133806E−05 −2.039078E−06 2.690957E−06 −4.389645E−06 −4.564835E−06 A16 1.531497E−08 1.511465E−07 1.312517E−06 9.781704E−08 −1.356427E−07 1.687907E−07 1.081353E−07 Surface 9 10 11 12 13 14 15 k −2.147168E+00 −1.417610E+00 −8.098865E−01 −1.349690E+00 1.523105E+01 −1.420397E−01 −4.247552E+00 A4 −2.757887E−03 4.473058E−02 3.215721E−02 −1.633779E−02 −7.157361E−03 −4.765358E−03 −4.148944E−03 A6 −3.779966E−03 −1.811946E−02 −9.953447E−03 2.870284E−03 2.430960E−03 1.500432E−03 4.018766E−04 A8 1.179723E−03 4.871273E−03 2.395917E−03 −4.751890E−04 −3.351483E−04 −1.853896E−04 −3.441282E−05 A10 −2.725621E−04 −8.658927E−04 −3.804019E−04 4.734240E−05 2.166505E−05 1.332742E−05 1.756637E−06 A12 3.800871E−05 9.274320E−05 3.621653E−05 −3.299378E−06 −7.320811E−07 −5.535770E−07 −5.226930E−08 A14 −2.865640E−06 −5.422388E−06 −1.817585E−06 1.287761E−07 1.263598E−08 1.204853E−08 8.341542E−10 A16 8.462583E−08 1.338454E−07 3.786058E−08 −2.240515E−09 −8.270280E−11 −1.054114E−10 −5.747740E−12

An equation of the aspheric surfaces of the second embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the second embodiment based on Table 3 and Table 4 are listed in the following table:

Second embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.7238 0.2602 0.5209 0.0905 0.3147 1.1403 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.9446 2.1860 1.1194 1.9528 0.0184 0.0589 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.1445 1.9707 3.8697 0.9631 HOS InTL HOS/HOI InS/HOS ODT % TDT % 10.9531 9.5145 1.4604 0.8256 28.8819 30.9635 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 1.7733 2.3058 2.5321 0.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 2.3739 0.0000 0.0000 2.9885 0.3985 0.2728 PSTA PLTA NSTA NLTA SSTA SLTA 0.009 −0.003 −0.00002 mm −0.003 mm 0.021 mm 0.002 mm mm mm

The figures related to the profile curve lengths obtained based on Table 3 and Table 4 are listed in the following table:

Second embodiment (Reference wavelength: 555 nm) ARE − 2(ARE/HEP) ARE ½(HEP) ARE value ½(HEP) % TP ARE/TP (%) 11 2.642 2.849 0.207 107.83% 1.702 167.37% 12 2.487 2.493 0.006 100.25% 1.702 146.46% 21 2.400 2.432 0.032 101.35% 0.300 810.73% 22 2.621 2.661 0.040 101.53% 0.300 886.90% 31 2.642 2.646 0.004 100.14% 1.172 225.73% 32 2.642 2.864 0.222 108.40% 1.172 244.36% 41 2.642 2.945 0.303 111.46% 0.478 616.03% 42 2.642 2.736 0.094 103.56% 0.478 572.38% 51 2.642 3.092 0.450 117.02% 0.662 466.83% 52 2.642 3.074 0.432 116.34% 0.662 464.13% 61 2.642 2.661 0.019 100.72% 1.300 204.66% 62 2.642 2.655 0.013 100.49% 1.300 204.20% 71 2.642 2.703 0.060 102.29% 0.581 464.98% 72 2.642 2.646 0.004 100.14% 0.581 455.21% ARS EHD ARS value ARS − EHD (ARS/EHD) % TP ARS/TP (%) 11 3.018 3.389 0.371 112.30% 1.702 199.08% 12 2.487 2.493 0.006 100.25% 1.702 146.46% 21 2.400 2.432 0.032 101.35% 0.300 810.73% 22 2.621 2.661 0.040 101.53% 0.300 886.90% 31 2.648 2.652 0.004 100.14% 1.172 226.24% 32 2.726 2.970 0.245 108.99% 1.172 253.42% 41 2.724 3.136 0.412 115.14% 0.478 656.06% 42 3.022 3.457 0.436 114.42% 0.478 723.22% 51 3.008 3.640 0.633 121.03% 0.662 549.63% 52 3.251 3.873 0.623 119.15% 0.662 584.80% 61 3.673 4.421 0.748 120.37% 1.300 340.01% 62 4.697 5.031 0.334 107.12% 1.300 386.92% 71 5.404 5.745 0.341 106.31% 0.581 988.40% 72 6.035 6.897 0.862 114.29% 0.581 1186.61% 

The results of the equations of the second embodiment based on Table 3 and Table 4 are listed in the following table:

Values related to the inflection points of the second embodiment (Reference wavelength: 555 nm) HIF211 0.9366 HIF211/HOI 0.1249 SGI211 0.0962 |SGI211|/(|SGI211| + TP2) 0.2427 HIF221 1.2605 HIF221/HOI 0.1681 SGI221 0.2081 |SGI221|/(|SGI221| + TP2) 0.4095 HIF222 2.5812 HIF222/HOI 0.3442 SGI222 0.3740 |SGI222|/(|SGI222| + TP2) 0.5549 HIF311 2.2429 HIF311/HOI 0.2990 SGI311 −0.0854 |SGI311|/(|SGI311| + TP3) 0.0679 HIF321 2.5873 HIF321/HOI 0.3450 SGI321 −0.8600 |SGI321|/(|SGI321| + TP3) 0.4232 HIF411 0.6530 HIF411/HOI 0.0871 SGI411 0.0152 |SGI411|/(|SGI411| + TP4) 0.0308 HIF421 0.8553 HIF421/HOI 0.1140 SGI421 0.0213 |SGI421|/(|SGI421| + TP4) 0.0426 HIF521 2.6973 HIF521/HOI 0.3596 SGI521 −1.4739 |SGI521|/(|SGI521| + TP5) 0.6900 HIF611 1.3749 HIF611/HOI 0.1833 SGI611 0.1494 |SGI611|/(|SGI611| + TP6) 0.1031 HIF621 4.0917 HIF621/HOI 0.5456 SGI621 −0.9661 |SGI621|/(|SGI621| + TP6) 0.4263 HIF622 4.6912 HIF622/HOI 0.6255 SGI622 −1.3669 |SGI622|/(|SGI622| + TP6) 0.5125 HIF711 4.9710 HIF711/HOI 0.6628 SGI711 −1.4770 |SGI711|/(|SGI711| + TP7) 0.7176 HIF712 5.4045 HIF712/HOI 0.7206 SGI712 −1.7430 |SGI712|/(|SGI712| + TP7) 0.7499 HIF721 1.5362 HIF721/HOI 0.2048 SGI721 0.0700 |SGI721|/(|SGI721| + TP7) 0.1075

Third Embodiment

As shown in FIG. 3A and FIG. 3B, an optical image capturing system of the third embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 310, an aperture 300, a second lens 320, a third lens 330, a fourth lens 340, a fifth lens 350, a sixth lens 360, a seventh lens 370, an infrared rays filter 380, an image plane 390, and an image sensor 392. FIG. 3C is a transverse aberration diagram at 0.7 field of view of the third embodiment of the present application.

The first lens 310 has positive refractive power and is made of plastic. An object-side surface 312 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 314 thereof, which faces the image side, is a concave aspheric surface.

The second lens 320 has negative refractive power and is made of plastic. An object-side surface 322 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 324 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 322 has an inflection point.

The third lens 330 has positive refractive power and is made of plastic. An object-side surface 332 thereof, which faces the object side, is a concave aspheric surface, and an image-side surface 334 thereof, which faces the image side, is a convex aspheric surface.

The fourth lens 340 has positive refractive power and is made of plastic. An object-side surface 342, which faces the object side, is a convex aspheric surface, and an image-side surface 344, which faces the image side, is a concave aspheric surface. The object-side surface 342 and the image-side surface 344 both have an inflection point.

The fifth lens 350 has negative refractive power and is made of plastic. An object-side surface 352, which faces the object side, is a concave aspheric surface, and an image-side surface 354, which faces the image side, is a convex aspheric surface The object-side surface 352 has two inflection points, and the image-side surface 354 has an inflection point.

The sixth lens 360 has positive refractive power and is made of plastic. An object-side surface 362, which faces the object side, is a convex surface, and an image-side surface 364, which faces the image side, is a convex surface. The object-side surface 362 has an inflection point, and the image-side surface 364 has four inflection points. Whereby, incident angle of each field of view for the sixth lens can be effectively adjusted to improve aberration.

The seventh lens 370 has negative refractive power and is made of plastic. An object-side surface 372, which faces the object side, is a concave surface, and an image-side surface 374, which faces the image side, is a concave surface. It may help to shorten the back focal length to keep small in size. In addition, the object-side surface 372 has two inflection points, and the image-side surface 374 has an inflection point, which may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 380 is made of glass and between the seventh lens 370 and the image plane 390. The infrared rays filter 390 gives no contribution to the focal length of the system.

In the third embodiment, the optical image capturing system of the third embodiment further satisfies ΣPP=78.5104 mm; and f1/ΣPP=0.1151, where ΣPP is a sum of the focal lengths of each positive lens. It is helpful to share the positive refractive power of one single lens to other positive lenses to avoid the significant aberration caused by the incident rays.

The optical image capturing system of the third embodiment further satisfies ΣNP=−45.7313 mm; and f7/ΣNP =0.1319, where ΣNP is a sum of the focal lengths of each negative lens. It is helpful to share the negative refractive power of the sixth lens 360 to other negative lenses.

The parameters of the lenses of the third embodiment are listed in Table 5 and Table 6.

TABLE 5 f = 9.5618 mm; f/HEP = 2.4; HAF = 37.5 deg Focal Radius of curvature Thickness Refractive Abbe length Surface (mm) (mm) Material index number (mm) 0 Object plane infinity 1 1^(st) lens 4.458622634 0.877 plastic 1.565 58.00 9.039 2 31.92259502 0.132 3 Aperture plane 0.486 4 2^(nd) lens 6.321588325 0.319 plastic 1.650 21.40 −19.494 5 4.144642961 0.676 6 3^(rd) lens −20.59925719 1.649 plastic 1.565 58.00 27.476 7 −9.125206377 0.182 8 4^(th) lens 10.94722522 0.393 plastic 1.565 58.00 33.702 9 25.31040695 1.394 10 5^(th) lens −2.265382263 0.494 plastic 1.650 21.40 −20.204 11 −2.968628844 0.057 12 6^(th) lens 6.501396026 1.324 plastic 1.583 30.20 8.293 13 −17.85062529 0.997 14 7^(th) lens −5.581859792 1.393 plastic 1.583 30.20 −6.034 15 10.55945401 1.000 16 Infrared plane 0.300 BK_7 1.517 64.2 rays filter 17 plane 0.423 18 Image plane 0.032 plane Reference wavelength (d-line): 555 nm.

TABLE 6 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k −6.769918E+00 −6.188364E+00 −5.000000E+01 −4.610981E+00 3.619848E+01 7.237748E+00 −6.435971E+00 A4 9.837048E−03 −2.042280E−03 2.517370E−03 −1.235437E−02 −1.138829E−03 −4.713368E−03 −5.984906E−03 A6 −1.028091E−03 5.748931E−04 −8.151008E−03 2.639372E−03 −3.002219E−04 −8.957672E−04 −2.516480E−03 A8 1.947168E−04 −4.338855E−05 4.869132E−03 −7.497695E−05 −2.687398E−04 7.039258E−04 1.292396E−03 A10 −3.693735E−05 −3.916043E−05 −1.644482E−03 −8.622551E−05 1.058477E−04 −2.523668E−04 −3.632848E−04 A12 7.032633E−06 2.055394E−05 3.290150E−04 1.925433E−05 −1.927678E−05 4.735523E−05 5.736779E−05 A14 −8.140090E−07 −4.306716E−06 −3.573085E−05 −1.506259E−06 3.547277E−07 −4.606171E−06 −4.642640E−06 A16 3.109772E−08 3.274301E−07 1.573251E−06 1.805685E−08 1.612013E−07 1.832176E−07 1.469521E−07 Surface 9 10 11 12 13 14 15 k −5.000000E+01 −1.126207E+00 −6.621843E−01 −8.901952E+00 1.137843E+01 −5.654885E−02 −6.181232E−01 A4 −9.357064E−04 4.514442E−02 2.856261E−02 −1.273411E−02 −6.416628E−03 −5.280222E−03 −5.381431E−03 A6 −3.040558E−03 −1.809690E−02 −1.009240E−02 3.050361E−03 2.448657E−03 1.523583E−03 4.360113E−04 A8 1.151924E−03 4.843654E−03 2.419435E−03 −5.107229E−04 −3.344984E−04 −1.838859E−04 −3.472939E−05 A10 −2.760117E−04 −8.632331E−04 −3.794917E−04 4.934688E−05 2.168603E−05 1.337660E−05 1.755233E−06 A12 3.872468E−05 9.340766E−05 3.615582E−05 −3.223107E−06 −7.308963E−07 −5.527811E−07 −5.233690E−08 A14 −2.791092E−06 −5.377363E−06 −1.828714E−06 1.292612E−07 1.260641E−08 1.203841E−08 8.353595E−10 A16 7.822557E−08 1.250015E−07 3.741685E−08 −2.293268E−09 −9.118725E−11 −1.078366E−10 −5.527053E−12

An equation of the aspheric surfaces of the third embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the third embodiment based on Table 5 and Table 6 are listed in the following table:

Third embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 1.0578 0.4905 0.3480 0.2837 0.4733 1.1531 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 1.5847 2.8426 2.5485 1.1154 0.0647 0.1043 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.4637 0.7095 4.6868 1.80552 HOS InTL HOS/HOI InS/HOS ODT % TDT %2 12.1287 10.3731 1.6172 0.9168 1.9999 1.09132 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 2.3701 0.0000 0.0000 2.9021 0.3870 0.2393 PSTA PLTA NSTA NLTA SSTA SLTA 0.009 mm 0.001 mm 0.003 mm −0.001 mm 0.005 mm 0.001 mm

The figures related to the profile curve lengths obtained based on Table 5 and Table 6 are listed in the following table:

Third embodiment (Reference wavelength: 555 nm) ARE − 2(ARE/HEP) ARE ½(HEP) ARE value ½(HEP) % TP ARE/TP (%) 11 1.992 2.069 0.077 103.86% 0.877 235.96% 12 1.992 1.993 0.001 100.04% 0.877 227.27% 21 1.992 1.997 0.005 100.24% 0.319 625.83% 22 1.992 2.024 0.032 101.58% 0.319 634.20% 31 1.992 2.004 0.012 100.61% 1.649 121.58% 32 1.992 2.032 0.040 102.01% 1.649 123.26% 41 1.992 1.994 0.002 100.09% 0.393 507.15% 42 1.992 1.993 0.001 100.05% 0.393 506.96% 51 1.992 2.112 0.120 106.01% 0.494 427.88% 52 1.992 2.080 0.088 104.44% 0.494 421.54% 61 1.992 2.000 0.008 100.38% 1.324 151.04% 62 1.992 1.997 0.005 100.27% 1.324 150.87% 71 1.992 2.042 0.050 102.52% 1.393 146.58% 72 1.992 1.997 0.004 100.22% 1.393 143.29% ARS EHD ARS value ARS − EHD (ARS/EHD) % TP ARS/TP (%) 11 2.251 2.367 0.116 105.16% 0.877 270.00% 12 2.036 2.036 0.000 100.01% 0.877 232.18% 21 2.086 2.091 0.005 100.22% 0.319 655.30% 22 2.192 2.230 0.038 101.75% 0.319 699.02% 31 2.222 2.247 0.025 101.14% 1.649 136.31% 32 2.762 2.974 0.212 107.66% 1.649 180.38% 41 2.998 3.079 0.081 102.70% 0.393 783.08% 42 3.150 3.237 0.086 102.74% 0.393 823.31% 51 3.247 3.625 0.378 111.65% 0.494 734.42% 52 3.509 3.836 0.327 109.32% 0.494 777.30% 61 3.938 4.323 0.385 109.77% 1.324 326.55% 62 4.884 5.087 0.203 104.16% 1.324 384.25% 71 5.207 5.533 0.326 106.26% 1.393 397.08% 72 6.358 7.077 0.719 111.30% 1.393 507.94%

The results of the equations of the third embodiment based on Table 5 and Table 6 are listed in the following table:

Values related to the inflection points of the third embodiment (Reference wavelength: 555 nm) HIF211 0.9746 HIF211/HOI 0.1299 SGI211 0.0590 |SGI211|/(|SGI211| + TP2) 0.1560 HIF411 0.9274 HIF411/HOI 0.1237 SGI411 0.0334 |SGI411|/(|SGI411| + TP4) 0.0784 HIF421 0.8439 HIF421/HOI 0.1125 SGI421 0.0126 |SGI421|/(|SGI421| + TP4) 0.0310 HIF511 2.5530 HIF511/HOI 0.3404 SGI511 −1.0094 |SGI511|/(|SGI511| + TP5) 0.6716 HIF512 3.0072 HIF512/HOI 0.4010 SGI512 −1.3198 |SGI512|/(|SGI512| + TP5) 0.7278 HIF521 2.6861 HIF521/HOI 0.3581 SGI521 −0.9666 |SGI521|/(|SGI521| + TP5) 0.6620 HIF611 1.2794 HIF611/HOI 0.1706 SGI611 0.0936 |SGI611|/(|SGI611| + TP6) 0.0660 HIF621 1.8102 HIF621/HOI 0.2414 SGI621 −0.1089 |SGI621|/(|SGI621| + TP6) 0.0760 HIF622 2.1205 HIF622/HOI 0.2827 SGI622 −0.1416 |SGI622|/(|SGI622| + TP6) 0.0966 HIF623 4.0505 HIF623/HOI 0.5401 SGI623 −0.6438 |SGI623|/(|SGI623| + TP6) 0.3272 HIF624 4.3558 HIF624/HOI 0.5808 SGI624 −0.7849 |SGI624|/(|SGI624| + TP6) 0.3722 HIF711 3.1387 HIF711/HOI 0.4185 SGI711 −0.9134 |SGI711|/(|SGI711| + TP7) 0.3960 HIF712 4.6732 HIF712/HOI 0.6231 SGI712 −1.5278 |SGI712|/(|SGI712| + TP7) 0.5230 HIF721 1.4794 HIF721/HOI 0.1973 SGI721 0.0819 |SGI721|/(|SGI721| + TP7) 0.0555

Fourth Embodiment

As shown in FIG. 4A and FIG. 4B, an optical image capturing system 40 of the fourth embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 410, an aperture 400, a second lens 420, a third lens 430, a fourth lens 440, a fifth lens 450, a sixth lens 460, a seventh lens 470, an infrared rays filter 480, an image plane 490, and an image sensor 492. FIG. 4C is a transverse aberration diagram at 0.7 field of view of the fourth embodiment of the present application.

The first lens 410 has positive refractive power and is made of plastic. An object-side surface 412 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 414 thereof, which faces the image side, is a concave aspheric surface.

The second lens 420 has negative refractive power and is made of plastic. An object-side surface 422 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 424 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 422 has an inflection point.

The third lens 430 has positive refractive power and is made of plastic. An object-side surface 432 thereof, which faces the object side, is a concave aspheric surface, and an image-side surface 434 thereof, which faces the image side, is a convex aspheric surface.

The fourth lens 440 has positive refractive power and is made of plastic. An object-side surface 442, which faces the object side, is a concave aspheric surface, and an image-side surface 444, which faces the image side, is a convex aspheric surface. The object-side surface 442 and the image-side surface 444 both have an inflection point.

The fifth lens 450 has negative refractive power and is made of plastic. An object-side surface 452, which faces the object side, is a concave aspheric surface, and an image-side surface 454, which faces the image side, is a convex aspheric surface. The object-side surface 452 has three inflection points, and the image-side surface 454 has an inflection point.

The sixth lens 460 has positive refractive power and is made of plastic. An object-side surface 462, which faces the object side, is a convex surface, and an image-side surface 464, which faces the image side, is a convex surface. The object-side surface 462 has an inflection point, and the object-side surface 464 has two inflection points. Whereby, incident angle of each field of view for the sixth lens can be effectively adjusted to improve aberration.

The seventh lens 470 has negative refractive power and is made of plastic. An object-side surface 472, which faces the object side, is a concave surface, and an image-side surface 474, which faces the image side, is a concave surface. It may help to shorten the back focal length to keep small in size. In addition, the object-side surface 472 has two inflection points, and the image-side surface 474 has an inflection point, which may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 480 is made of glass and between the seventh lens 470 and the image plane 490. The infrared rays filter 480 gives no contribution to the focal length of the system.

In the fourth embodiment, the optical image capturing system of the fourth embodiment further satisfies ΣPP=78.8784 mm; and f1/ΣPP=0.1113, where ΣPP is a sum of the focal lengths of each positive lens. It is helpful to share the positive refractive power of one single lens to other positive lenses to avoid the significant aberration caused by the incident rays.

The optical image capturing system of the fourth embodiment further satisfies ΣNP=−42.9439 mm; and f7/ΣNP=0.1363, where ΣNP is a sum of the focal lengths of each negative lens. It is helpful to share the negative refractive power of one single lens to other negative lenses.

The parameters of the lenses of the fourth embodiment are listed in Table 7 and Table 8.

TABLE 7 f = 9.5666 mm; f/HEP = 2.8; HAF = 37.5 deg Focal Radius of curvature Thickness Refractive Abbe length Surface (mm) (mm) Material index number (mm) 0 Object plane infinity 1 1^(st) lens 4.788559965 0.728 plastic 1.565 58.00 8.775 2 121.5515646 0.108 3 Aperture plane 0.425 4 2^(nd) lens 6.563453471 0.353 plastic 1.650 21.40 −18.156 5 4.140212814 0.686 6 3^(rd) lens −15.64535928 1.318 plastic 1.565 58.00 40.219 7 −9.560449295 0.449 8 4^(th) lens −26.50102493 0.681 plastic 1.565 58.00 21.587 9 −8.448471717 1.275 10 5^(th) lens −2.3703115 0.458 plastic 1.650 21.40 −18.933 11 −3.154082475 0.260 12 6^(th) lens 6.350358479 1.224 plastic 1.583 30.20 8.297 13 −19.33348548 1.128 14 7^(th) lens −5.556630688 1.387 plastic 1.583 30.20 −5.855 15 9.81809086 1.000 16 Infrared plane 0.300 BK_7 1.517 64.2 rays filter 17 plane 0.421 18 Image plane 0.027 plane Reference wavelength (d-line): 555 nm.

TABLE 8 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k −8.541451E+00 5.000000E+01 −5.000000E+01 −1.255860E+00 3.438780E+01 1.037012E+01 5.000000E+01 A4 1.054197E−02 1.458164E−04 7.218547E−03 −1.329818E−02 −3.083862E−03 −4.374156E−03 −6.951863E−03 A6 −1.095839E−03 4.265172E−04 −8.070234E−03 2.322558E−03 −1.147034E−04 −8.820916E−04 −2.543939E−03 A8 1.593040E−04 −1.125463E−04 4.485382E−03 −2.002043E−04 −1.578306E−04 7.109484E−04 1.290083E−03 A10 −1.021325E−05 −6.667591E−07 −1.623724E−03 −5.609750E−05 5.573740E−05 −2.462473E−04 −3.645877E−04 A12 5.847968E−06 2.186462E−05 3.553178E−04 2.358188E−05 −1.417555E−05 4.756165E−05 5.753038E−05 A14 −2.275257E−06 −8.495319E−06 −3.942184E−05 −1.810874E−06 1.976971E−06 −4.611415E−06 −4.629210E−06 A16 2.721299E−07 1.040794E−06 1.370809E−06 −1.298768E−07 −1.119901E−07 1.685553E−07 1.516391E−07 Surface 9 10 11 12 13 14 15 k 5.330959E+00 −1.196341E+00 −6.824307E−01 −6.404575E+00 1.484850E+01 −5.580928E−02 −2.903132E−01 A4 −8.044999E−04 4.578808E−02 2.909557E−02 −1.322926E−02 −6.285271E−03 −5.164617E−03 −5.610506E−03 A6 −3.038872E−03 −1.803425E−02 −1.009390E−02 3.112061E−03 2.449247E−03 1.520939E−03 4.474495E−04 A8 1.141016E−03 4.834947E−03 2.420551E−03 −5.106637E−04 −3.348453E−04 −1.839025E−04 −3.491290E−05 A10 −2.772937E−04 −8.645702E−04 −3.797089E−04 4.934527E−05 2.166639E−05 1.337651E−05 1.753545E−06 A12 3.833665E−05 9.332471E−05 3.611415E−05 −3.220971E−06 −7.315875E−07 −5.527936E−07 −5.231885E−08 A14 −2.807598E−06 −5.374714E−06 −1.831530E−06 1.291317E−07 1.259274E−08 1.203746E−08 8.361821E−10 A16 9.023221E−08 1.260842E−07 3.774371E−08 −2.360800E−09 −9.081864E−11 −1.079155E−10 −5.517533E−12

An equation of the aspheric surfaces of the fourth embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the fourth embodiment based on Table 7 and Table 8 are listed in the following table:

Fourth embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 1.0902 0.5269 0.2379 0.4432 0.5053 1.1530 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 1.6339 2.9242 2.6661 1.0968 0.0557 0.1179 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.4833 0.4514 3.5722 2.05472 HOS InTL HOS/HOI InS/HOS ODT % TDT %2 12.2277 10.4799 1.6304 0.9317 2.0000 1.18252 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 2.4666 0.0000 0.0000 3.0243 0.4032 0.2473 PSTA PLTA NSTA NLTA SSTA SLTA 0.009 mm −0.002 0.003 mm −0.00017 mm 0.003 mm 0.001 mm mm

The figures related to the profile curve lengths obtained based on Table 7 and Table 8 are listed in the following table:

Fourth embodiment (Reference wavelength: 555 nm) ARE − 2(ARE/HEP) ARE ½(HEP) ARE value ½(HEP) % TP ARE/TP (%) 11 1.708 1.750 0.042 102.44% 0.728 240.50% 12 1.708 1.708 −0.00013 99.99% 0.728 234.76% 21 1.708 1.715 0.007 100.39% 0.353 485.90% 22 1.708 1.735 0.027 101.59% 0.353 491.72% 31 1.708 1.717 0.009 100.52% 1.318 130.27% 32 1.708 1.727 0.018 101.08% 1.318 130.99% 41 1.708 1.718 0.010 100.56% 0.681 252.19% 42 1.708 1.730 0.022 101.27% 0.681 253.98% 51 1.708 1.776 0.068 103.96% 0.458 387.80% 52 1.708 1.755 0.047 102.74% 0.458 383.26% 61 1.708 1.715 0.007 100.41% 1.224 140.16% 62 1.708 1.711 0.003 100.17% 1.224 139.82% 71 1.708 1.740 0.032 101.85% 1.387 125.45% 72 1.708 1.712 0.004 100.23% 1.387 123.45% ARS EHD ARS value ARS − EHD (ARS/EHD) % TP ARS/TP (%) 11 1.971 2.039 0.069 103.48% 0.728 280.24% 12 1.767 1.766 −0.00035 99.98% 0.728 242.73% 21 1.869 1.876 0.007 100.36% 0.353 531.44% 22 1.979 2.017 0.038 101.93% 0.353 571.62% 31 2.039 2.064 0.025 101.21% 1.318 156.58% 32 2.567 2.694 0.127 104.94% 1.318 204.35% 41 2.758 2.885 0.127 104.62% 0.681 423.57% 42 2.902 3.174 0.273 109.40% 0.681 466.01% 51 3.230 3.563 0.333 110.31% 0.458 778.07% 52 3.503 3.760 0.257 107.34% 0.458 821.15% 61 3.936 4.388 0.452 111.48% 1.224 358.53% 62 4.742 5.066 0.324 106.84% 1.224 413.95% 71 5.201 5.547 0.346 106.65% 1.387 399.91% 72 6.445 7.128 0.684 110.61% 1.387 513.95%

The results of the equations of the fourth embodiment based on Table 7 and Table 8 are listed in the following table:

Values related to the inflection points of the fourth embodiment (Reference wavelength: 555 nm) HIF211 1.2844 HIF211/HOI 0.1712 SGI211 0.0959 |SGI211|/(|SGI211| + TP2) 0.2137 HIF411 2.6305 HIF411/HOI 0.3507 SGI411 −0.5590 |SGI411|/(|SGI411| + TP4) 0.4507 HIF421 2.7033 HIF421/HOI 0.3604 SGI421 −0.8491 |SGI421|/(|SGI421| + TP4) 0.5549 HIF511 2.6892 HIF511/HOI 0.3586 SGI511 −1.0098 |SGI511|/(|SGI511| + TP5) 0.6880 HIF512 2.9994 HIF512/HOI 0.3999 SGI512 −1.2196 |SGI512|/(|SGI512| + TP5) 0.7270 HIF513 3.1429 HIF513/HOI 0.4191 SGI513 −1.3157 |SGI513|/(|SGI513| + TP5) 0.7418 HIF521 2.6929 HIF521/HOI 0.3591 SGI521 −0.8562 |SGI521|/(|SGI521| + TP5) 0.6515 HIF611 1.3753 HIF611/HOI 0.1834 SGI611 0.1088 |SGI611|/(|SGI611| + TP6) 0.0816 HIF621 1.7184 HIF621/HOI 0.2291 SGI621 −0.0917 |SGI621|/(|SGI621| + TP6) 0.0697 HIF622 2.1923 HIF622/HOI 0.2923 SGI622 −0.1360 |SGI622|/(|SGI622| + TP6) 0.1000 HIF711 3.1340 HIF711/HOI 0.4179 SGI711 −0.9079 |SGI711|/(|SGI711| + TP7) 0.3956 HIF712 4.5559 HIF712/HOI 0.6075 SGI712 −1.4952 |SGI712|/(|SGI712| + TP7) 0.5188 HIF721 1.5264 HIF721/HOI 0.2035 SGI721 0.0935 |SGI721|/(|SGI721| + TP7) 0.0631

Fifth Embodiment

As shown in FIG. 5A and FIG. 5B, an optical image capturing system of the fifth embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 510, an aperture 500, a second lens 520, a third lens 530, a fourth lens 540, a fifth lens 550, a sixth lens 560, a seventh lens 570, an infrared rays filter 580, an image plane 590, and an image sensor 592. FIG. 5C is a transverse aberration diagram at 0.7 field of view of the fifth embodiment of the present application.

The first lens 510 has positive refractive power and is made of plastic. An object-side surface 512, which faces the object side, is a convex aspheric surface, and an image-side surface 514, which faces the image side, is a concave aspheric surface.

The second lens 520 has negative refractive power and is made of plastic. An object-side surface 522 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 524 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 552 and the image-side surface 524 both have an inflection point.

The third lens 530 has positive refractive power and is made of plastic. An object-side surface 532, which faces the object side, is a convex aspheric surface, and an image-side surface 534, which faces the image side, is a convex aspheric surface. The object-side surface 532 has two inflection points.

The fourth lens 540 has positive refractive power and is made of plastic.

An object-side surface 542, which faces the object side, is a convex aspheric surface, and an image-side surface 544, which faces the image side, is a convex aspheric surface. The object-side surface 542 has an inflection point.

The fifth lens 550 has negative refractive power and is made of plastic. An object-side surface 552, which faces the object side, is a concave aspheric surface, and an image-side surface 554, which faces the image side, is a concave aspheric surface. The object-side surface 552 has two inflection points, and the image-side surface 554 has an inflection point.

The sixth lens 560 can have positive refractive power and is made of plastic. An object-side surface 562, which faces the object side, is a convex surface, and an image-side surface 564, which faces the image side, is a convex surface. The object-side surface 562 has two inflection points, and the image-side surface 564 has three inflection points. Whereby, incident angle of each field of view for the sixth lens 560 can be effectively adjusted to improve aberration.

The seventh lens 570 has negative refractive power and is made of plastic. An object-side surface 572, which faces the object side, is a concave surface, and an image-side surface 574, which faces the image side, is a concave surface. It may help to shorten the back focal length to keep small in size. In addition, the object-side surface 572 has two inflection points, and the image-side surface 574 has an inflection point, which may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 580 is made of glass and between the seventh lens 570 and the image plane 590. The infrared rays filter 580 gives no contribution to the focal length of the system.

In the fifth embodiment, the optical image capturing system of the fifth embodiment further satisfies ΣPP=77.0412 mm; and f1/ΣPP=0.1705, where ΣPP is a sum of the focal lengths of each positive lens. It is helpful to share the positive refractive power of one single lens to other positive lenses to avoid the significant aberration caused by the incident rays.

The optical image capturing system of the fifth embodiment further satisfies ΣNP=−162.0436 mm; and f7/ΣNP=0.0429, where ΣNP is a sum of the focal lengths of each negative lens. It is helpful to share the negative refractive power of one single lens to other negative lenses.

The parameters of the lenses of the fifth embodiment are listed in Table 9 and Table 10.

TABLE 9 f = 6.5733 mm; f/HEP = 1.4; HAF = 42.5 deg Focal Radius of curvature Thickness Refractive Abbe length Surface (mm) (mm) Material index number (mm) 0 Object plane infinity 1 1^(st) lens 5.446364908 1.040 plastic 1.565 58.00 13.139 2 18.87365407 0.121 3 Aperture plane 0.000 4 2^(nd) lens 3.396487656 0.300 plastic 1.650 21.40 −90.957 5 3.101036314 0.471 6 3^(rd) lens 1111.885105 0.771 plastic 1.565 54.50 46.154 7 −26.78814758 0.468 8 4^(th) lens 21.12493198 1.022 plastic 1.565 58.00 10.650 9 −8.303556039 0.829 10 5^(th) lens −1.857091195 1.420 plastic 1.650 21.40 −64.128 11 −2.531101729 0.050 12 6^(th) lens 4.26425423 1.222 plastic 1.565 58.00 7.098 13 −63.72206001 0.387 14 7^(th) lens −23.65770031 0.790 plastic 1.650 21.40 −6.959 15 5.725020915 1.000 16 Infrared plane 0.300 BK_7 1.517 64.2 rays filter 17 plane 0.715 18 Image plane 0.031 plane Reference wavelength (d-line): 555 nm; the position of blocking light: blocking at the first surface with effective semi diameter of 2.750 mm; blocking at the seventh surface with effective semi diameter of 2.500 mm.

TABLE 10 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k 3.602747E−01 3.097617E+01 −4.914929E+00 −9.449708E−01 −5.000000E+01 5.000000E+01 −4.178150E+00 A4 1.025175E−03 −8.694810E−03 −8.340919E−03 −1.113956E−02 −1.649846E−03 −1.101535E−02 −1.191129E−02 A6 3.415693E−04 3.302085E−03 −1.258698E−03 −3.166952E−03 1.102903E−03 −4.039507E−04 −2.494873E−03 A8 −2.962521E−04 −1.244063E−03 −1.161113E−03 3.628299E−04 −3.720513E−04 6.241343E−04 9.331250E−04 A10 9.802308E−05 3.390037E−04 6.982355E−04 1.591186E−04 4.959135E−05 −2.789218E−04 −4.023604E−04 A12 −1.674386E−05 −5.833077E−05 −1.577616E−04 −5.487693E−05 −8.662730E−06 6.243935E−05 9.060507E−05 A14 1.465645E−06 5.546200E−06 1.675460E−05 5.980045E−06 1.396475E−06 −6.722999E−06 −1.061610E−05 A16 −5.229988E−08 −2.210286E−07 −7.061959E−07 −1.960326E−07 −6.322729E−08 2.776015E−07 4.736098E−07 Surface 9 10 11 12 13 14 15 k −2.888377E+01 −6.539364E−01 −5.980761E−01 −1.326514E+01 −4.269993E+01 9.240303E+00 −1.121151E+01 A4 −9.835062E−03 2.945936E−02 7.060393E−03 1.838522E−03 −6.822278E−03 6.993184E−03 8.517562E−03 A6 −1.122282E−03 −7.400431E−03 −2.559604E−04 −8.947241E−04 3.419590E−03 −5.371355E−05 −1.823942E−03 A8 1.245332E−04 2.084361E−03 −2.804894E−05 2.008524E−04 −5.633828E−04 −1.823336E−04 1.657220E−04 A10 −5.996834E−05 −4.046282E−04 2.586716E−05 −2.845687E−05 4.282588E−05 2.332620E−05 −8.391854E−06 A12 1.402146E−05 5.840699E−05 −3.712356E−06 1.890028E−06 −1.737673E−06 −1.315443E−06 2.409729E−07 A14 −1.214827E−06 −4.740857E−06 2.391870E−07 −5.732399E−08 3.700734E−08 3.640479E−08 −3.661828E−09 A16 2.793602E−08 1.581652E−07 −5.607171E−09 6.541259E−10 −3.242797E−10 −4.077483E−10 2.277145E−11

An equation of the aspheric surfaces of the fifth embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the fifth embodiment based on Table 9 and Table 10 are listed in the following table:

Fifth embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.5003 0.0723 0.1424 0.6172 0.1025 0.9261 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.9446 2.1860 1.1194 1.9528 0.0184 0.0589 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.1445 1.9707 3.8697 0.96312 HOS InTL HOS/HOI InS/HOS ODT % TDT %2 10.9367 8.8907 1.4582 0.8938 24.0649 14.42582 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 1.8837 2.2022 0.4002 0.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 2.9336 0.0000 0.0000 4.2652 0.5687 0.3900 PSTA PLTA NSTA NLTA SSTA SLTA 0.010 mm −0.005 −0.006 mm −0.006 mm 0.019 mm 0.010 mm mm

The figures related to the profile curve lengths obtained based on Table 9 and Table 10 are listed in the following table:

Fifth embodiment (Reference wavelength: 555 nm) ARE ½(HEP) ARE value ARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 2.348 2.440 0.09192 103.92% 1.040 234.58% 12 2.348 2.348 0.00054 100.02% 1.040 225.80% 21 2.277 2.301 0.02435 101.07% 0.300 767.01% 22 2.348 2.390 0.04243 101.81% 0.300 796.67% 31 2.348 2.348 0.00020 100.01% 0.771 304.35% 32 2.348 2.413 0.06536 102.78% 0.771 312.79% 41 2.348 2.518 0.17008 107.25% 1.022 246.46% 42 2.348 2.514 0.16634 107.09% 1.022 246.09% 51 2.348 2.702 0.35456 115.10% 1.420 190.31% 52 2.348 2.599 0.25112 110.70% 1.420 183.02% 61 2.348 2.386 0.03828 101.63% 1.222 195.25% 62 2.348 2.347 −0.00023 99.99% 1.222 192.10% 71 2.348 2.347 −0.00021 99.99% 0.790 297.22% 72 2.348 2.396 0.04875 102.08% 0.790 303.42% ARS EHD ARS value ARS − EHD (ARS/EHD) % TP ARS/TP (%) 11 2.678 2.823 0.14550 105.43% 1.040 271.47% 12 2.394 2.394 0.00036 100.02% 1.040 230.22% 21 2.277 2.301 0.02435 101.07% 0.300 767.01% 22 2.407 2.449 0.04229 101.76% 0.300 816.39% 31 2.428 2.428 0.00015 100.01% 0.771 314.72% 32 2.500 2.592 0.09166 103.67% 0.771 335.96% 41 2.518 2.863 0.34423 113.67% 1.022 280.23% 42 2.825 3.352 0.52701 118.66% 1.022 328.11% 51 2.899 3.398 0.49919 117.22% 1.420 239.32% 52 3.454 3.907 0.45280 113.11% 1.420 275.15% 61 4.708 4.859 0.15082 103.20% 1.222 397.62% 62 4.794 4.978 0.18390 103.84% 1.222 407.39% 71 4.819 5.234 0.41482 108.61% 0.790 662.74% 72 6.306 6.797 0.49164 107.80% 0.790 860.66%

The results of the equations of the fifth embodiment based on Table 9 and Table 10 are listed in the following table:

Values related to the inflection points of the fifth embodiment (Reference wavelength: 555 nm) HIF211 1.0559 HIF211/HOI 0.1408 SGI211 0.1380 |SGI211|/(|SGI211| + TP2) 0.3151 HIF221 1.2431 HIF221/HOI 0.1657 SGI221 0.2143 |SGI221|/(|SGI221| + TP2) 0.4166 HIF311 0.2221 HIF311/HOI 0.0296 SGI311 0.00002 |SGI311|/(|SGI311| + TP3) 0.00002 HIF312 2.1666 HIF312/HOI 0.2889 SGI312 −0.0252 |SGI312|/(|SGI312| + TP3) 0.0317 HIF411 0.5411 HIF411/HOI 0.0722 SGI411 0.0058 |SGI411|/(|SGI411| + TP4) 0.0057 HIF511 2.1614 HIF511/HOI 0.2882 SGI511 −1.0614 |SGI511|/(|SGI511| + TP5) 0.4278 HIF512 2.7106 HIF512/HOI 0.3614 SGI512 −1.4982 |SGI512|/(|SGI512| + TP5) 0.5134 HIF521 2.5210 HIF521/HOI 0.3361 SGI521 −1.1318 |SGI521|/(|SGI521| + TP5) 0.4435 HIF611 1.8550 HIF611/HOI 0.2473 SGI611 0.2885 |SGI611|/(|SGI611| + TP6) 0.1910 HIF612 3.8589 HIF612/HOI 0.5145 SGI612 0.1827 |SGI612|/(|SGI612| + TP6) 0.1301 HIF621 1.1967 HIF621/HOI 0.1596 SGI621 −0.0173 |SGI621|/(|SGI621| + TP6) 0.0139 HIF622 2.2074 HIF622/HOI 0.2943 SGI622 −0.0250 |SGI622|/(|SGI622| + TP6) 0.0201 HIF623 4.0580 HIF623/HOI 0.5411 SGI623 −0.5252 |SGI623|/(|SGI623| + TP6) 0.3006 HIF711 0.7303 HIF711/HOI 0.0974 SGI711 −0.0093 |SGI711|/(|SGI711| + TP7) 0.0117 HIF712 1.9781 HIF712/HOI 0.2637 SGI712 −0.0060 |SGI712|/(|SGI712| + TP7) 0.0075 HIF721 2.0688 HIF721/HOI 0.2758 SGI721 0.3537 |SGI721|/(|SGI721| + TP7) 0.3093

Sixth Embodiment

As shown in FIG. 6A and FIG. 6B, an optical image capturing system of the sixth embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 610, an aperture 600, a second lens 620, a third lens 630, a fourth lens 640, a fifth lens 650, a seventh lens 660, a seventh lens 670, an infrared rays filter 680, an image plane 690, and an image sensor 692. FIG. 6C is a transverse aberration diagram at 0.7 field of view of the sixth embodiment of the present application.

The first lens 610 has positive refractive power and is made of plastic. An object-side surface 612, which faces the object side, is a convex aspheric surface, and an image-side surface 614, which faces the image side, is a concave aspheric surface.

The second lens 620 has negative refractive power and is made of plastic. An object-side surface 622 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 624 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 612 and the image-side surface 614 both have an inflection point.

The third lens 630 has positive refractive power and is made of plastic. An object-side surface 632, which faces the object side, is a convex aspheric surface, and an image-side surface 634, which faces the image side, is a convex aspheric surface. The object-side surface 632 has an inflection point.

The fourth lens 640 has positive refractive power and is made of plastic. An object-side surface 642, which faces the object side, is a concave aspheric surface, and an image-side surface 644, which faces the image side, is a convex aspheric surface.

The fifth lens 650 has positive refractive power and is made of plastic. An object-side surface 652, which faces the object side, is a concave aspheric surface, and an image-side surface 654, which faces the image side, is a convex aspheric surface. The object-side surface 652 has two inflection points, and the image-side surface 654 has an inflection point.

The sixth lens 660 can have positive refractive power and is made of plastic. An object-side surface 662, which faces the object side, is a convex surface, and an image-side surface 664, which faces the image side, is a convex surface. The object-side surface 662 has an inflection point, and the image-side surface 664 both have two inflection points. Whereby, incident angle of each field of view for the sixth lens 660 can be effectively adjusted to improve aberration.

The seventh lens 670 has negative refractive power and is made of plastic. An object-side surface 672, which faces the object side, is a concave surface, and an image-side surface 674, which faces the image side, is a concave surface. The image-side surface 664 has an inflection point. It may help to shorten the back focal length to keep small in size. In addition, it may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 680 is made of glass and between the seventh lens 670 and the image plane 690. The infrared rays filter 680 gives no contribution to the focal length of the system.

In the sixth embodiment, the optical image capturing system of the sixth embodiment further satisfies ΣPP=126.2162 mm; and f1/ΣPP=0.1279, where ΣPP is a sum of the focal lengths of each positive lens. It is helpful to share the positive refractive power of one single lens to other positive lenses to avoid the significant aberration caused by the incident rays.

The optical image capturing system of the sixth embodiment further satisfies ΣNP=−67.2059 mm; and f7/ΣNP=0.0439, where ΣNP is a sum of the focal lengths of each negative lens. It is helpful to share the negative refractive power of one single lens to the other negative lenses to avoid the significant aberration caused by the incident rays.

The parameters of the lenses of the sixth embodiment are listed in Table 11 and Table 12.

TABLE 11 f = 5.5641 mm; f/HEP = 1.4, HAF = 47.4997 deg Focal Radius of curvature Thickness Refractive Abbe length Surface (mm) (mm) Material index number (mm) 0 Object plane infinity 1 1^(st) lens 4.835295814 0.900 plastic 1.583 30.20 16.143 2 9.202478641 0.285 3 Aperture plane 0.000 4 2^(nd) lens 3.441455186 0.300 plastic 1.650 21.40 −64.253 5 3.071668034 0.224 6 3^(rd) lens 23.31186563 0.956 plastic 1.565 58.00 9.049 7 −6.477580922 0.444 8 4^(th) lens −17.052696 0.683 plastic 1.583 30.20 32.205 9 −9.094338954 0.484 10 5^(th) lens −1.774149519 1.310 plastic 1.650 21.40 65.478 11 −2.201644982 0.050 12 6^(th) lens 4.867708036 1.710 plastic 1.565 58.00 3.341 13 −2.705046837 0.050 14 7^(th) lens −494.7308627 0.319 plastic 1.632 23.40 −2.953 15 1.888118555 1.000 16 Infrared plane 0.300 BK_7 1.517 64.2 rays filter 17 plane 0.844 18 Image plane 0.030 plane Reference wavelength (d-line): 555 nm; the position of blocking light: blocking at the fifth surface with effective semi diameter of 1.800 mm.

TABLE 12 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k 2.768284E+00 −5.000000E+01 −1.035316E+01 −8.272938E−02 3.601860E+01 7.814113E+00 4.524743E+01 A4 −1.475794E−03 −1.088211E−03 −5.308306E−03 −2.364538E−02 4.629937E−03 −9.146872E−03 −2.590179E−02 A6 −2.331608E−04 2.062780E−03 −1.187216E−02 −5.094192E−03 2.194458E−04 −1.315089E−03 −1.117375E−03 A8 −4.121856E−05 −8.257885E−04 3.585864E−03 2.778677E−03 5.904392E−04 1.721749E−03 1.799055E−04 A10 1.938112E−05 2.459819E−04 −4.421450E−04 −6.203167E−04 −3.772064E−04 −6.934823E−04 1.170661E−05 A12 −4.307645E−06 −3.183023E−05 −8.389137E−07 8.042273E−05 8.304326E−05 1.461540E−04 −8.184639E−06 A14 −1.796938E−07 −2.247683E−06 2.054647E−06 −9.987278E−06 −1.015623E−05 −1.374920E−05 2.951361E−06 A16 5.534772E−08 9.836096E−07 −1.372780E−07 −1.233460E−07 −1.487042E−07 5.950855E−07 −1.618381E−06 Surface 9 10 11 12 13 14 15 k −1.024500E+00 −5.565418E−01 −6.036603E−01 4.086985E−02 −2.098867E+01 5.000000E+01 −6.302732E+00 A4 −1.978975E−02 2.414207E−02 1.317775E−02 −1.104408E−02 −5.902830E−03 −8.544737E−03 −5.130267E−03 A6 −1.703764E−03 −6.364618E−03 −2.350597E−03 1.594649E−03 2.891567E−03 1.563878E−03 4.397092E−04 A8 −1.278484E−05 1.339730E−03 5.627750E−04 −1.783258E−04 −3.862756E−04 −1.634816E−04 −2.936151E−05 A10 −2.950492E−05 −6.883022E−05 −5.960294E−05 9.891271E−06 2.474392E−05 9.876828E−06 1.303617E−06 A12 1.818520E−05 1.340413E−05 5.877376E−06 −3.399782E−07 −8.467402E−07 −3.371806E−07 −3.620071E−08 A14 −1.042020E−06 −1.827701E−06 −3.791703E−07 8.475571E−09 1.489296E−08 5.979359E−09 5.537102E−10 A16 −3.109811E−07 8.816615E−08 1.052032E−08 −1.363672E−10 −1.069406E−10 −4.271087E−11 −3.571421E−12

An equation of the aspheric surfaces of the sixth embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the sixth embodiment based on Table 11 and

Table 12 are listed in the following table:

Sixth embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.3447 0.0866 0.6149 0.1728 0.0850 1.6655 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 1.8844 2.8829 1.9710 1.4627 0.0512 0.0090 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.2512 7.1009 3.9501 0.21592 HOS InTL HOS/HOI InS/HOS ODT % TDT %2 9.8889 7.7147 1.3185 0.8802 23.1027 15.11462 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 1.4514 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 3.4244 0.0000 0.0000 4.0945 0.5459 0.4140 PSTA PLTA NSTA NLTA SSTA SLTA −0.025 mm −0.003 mm 0.043 0.032 mm 0.004 mm 0.002 mm mm

The figures related to the profile curve lengths obtained based on Table 11 and Table 12 are listed in the following table:

Sixth embodiment (Reference wavelength: 555 nm) ARE ½(HEP) ARE value ARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.987 2.061 0.074 103.73% 0.900 229.03% 12 1.987 2.002 0.015 100.75% 0.900 222.45% 21 1.817 1.831 0.014 100.75% 0.300 610.23% 22 1.800 1.827 0.027 101.51% 0.300 609.03% 31 1.856 1.861 0.005 100.28% 0.956 194.69% 32 1.987 2.090 0.103 105.19% 0.956 218.70% 41 1.987 2.187 0.200 110.07% 0.683 320.46% 42 1.987 2.157 0.170 108.54% 0.683 316.00% 51 1.987 2.316 0.329 116.55% 1.310 176.85% 52 1.987 2.192 0.205 110.32% 1.310 167.40% 61 1.987 2.018 0.030 101.53% 1.710 117.96% 62 1.987 2.015 0.028 101.39% 1.710 117.80% 71 1.987 1.989 0.002 100.11% 0.319 623.08% 72 1.987 2.061 0.074 103.72% 0.319 645.52% ARS EHD ARS value ARS − EHD (ARS/EHD) % TP ARS/TP (%) 11 2.426 2.642 0.217 108.93% 0.900 293.59% 12 2.046 2.066 0.019 100.95% 0.900 229.51% 21 1.817 1.831 0.014 100.75% 0.300 610.23% 22 1.800 1.827 0.027 101.51% 0.300 609.03% 31 1.856 1.861 0.005 100.28% 0.956 194.69% 32 2.009 2.117 0.108 105.37% 0.956 221.48% 41 2.073 2.372 0.299 114.43% 0.683 347.49% 42 2.320 2.814 0.494 121.28% 0.683 412.20% 51 2.399 2.867 0.468 119.50% 1.310 218.92% 52 3.053 3.430 0.376 112.32% 1.310 261.88% 61 4.544 4.833 0.290 106.37% 1.710 282.59% 62 5.214 5.469 0.254 104.88% 1.710 319.73% 71 5.464 5.613 0.149 102.73% 0.319 1757.96% 72 6.338 6.893 0.555 108.75% 0.319 2158.95%

The results of the equations of the sixth embodiment based on Table 11 and Table 12 are listed in the following table:

Values related to the inflection points of the sixth embodiment (Reference wavelength: 555 nm) HIF211 0.8235 HIF211/HOI 0.1098 SGI211 0.0825 |SGI211|/(|SGI211| + TP2) 0.2158 HIF221 1.1073 HIF221/HOI 0.1476 SGI221 0.1658 |SGI221|/(|SGI221| + TP2) 0.3559 HIF311 1.5989 HIF311/HOI 0.2132 SGI311 0.0911 |SGI311|/(|SGI311| + TP3) 0.0870 HIF511 1.9364 HIF511/HOI 0.2582 SGI511 −1.0136 |SGI511|/(|SGI511| + TP5) 0.4363 HIF512 2.3698 HIF512/HOI 0.3160 SGI512 −1.4047 |SGI512|/(|SGI512| + TP5) 0.5175 HIF521 2.1173 HIF521/HOI 0.2823 SGI521 −0.9258 |SGI521|/(|SGI521| + TP5) 0.4141 HIF611 2.3238 HIF611/HOI 0.3098 SGI611 0.4076 |SGI611|/(|SGI611| + TP6) 0.1925 HIF621 1.248 HIF621/HOI 0.1665 SGI621 −0.1805 |SGI621|/(|SGI621| + TP6) 0.0955 HIF622 2.8784 HIF622/HOI 0.3838 SGI622 −0.3737 |SGI622|/(|SGI622| + TP6) 0.1793 HIF721 1.3346 HIF721/HOI 0.1779 SGI721 0.3101 |SGI721|/(|SGI721| + TP7) 0.4927

Seventh Embodiment

As shown in FIG. 7A and FIG. 7B, an optical image capturing system of the seventh embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 710, an aperture 700, a second lens 720, a third lens 730, a fourth lens 740, a fifth lens 750, a seventh lens 760, a seventh lens 770, an infrared rays filter 780, an image plane 790, and an image sensor 792. FIG. 7C is a transverse aberration diagram at 0.7 field of view of the seventh embodiment of the present application.

The first lens 710 has positive refractive power and is made of plastic. An object-side surface 712, which faces the object side, is a convex aspheric surface, and an image-side surface 714, which faces the image side, is a concave aspheric surface.

The second lens 720 has negative refractive power and is made of plastic. An object-side surface 722 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 724 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 722 has an inflection point.

The third lens 730 has positive refractive power and is made of plastic. An object-side surface 732, which faces the object side, is a concave surface, and an image-side surface 734, which faces the image side, is a convex surface.

The fourth lens 740 has positive refractive power and is made of plastic. An object-side surface 742, which faces the object side, is a concave aspheric surface, and an image-side surface 744, which faces the image side, is a convex aspheric surface.

The fifth lens 750 has negative refractive power and is made of plastic. An object-side surface 752, which faces the object side, is a concave aspheric surface, and an image-side surface 754, which faces the image side, is a convex aspheric surface. The image-side surface 754 has an inflection point.

The sixth lens 760 can have positive refractive power and is made of plastic. An object-side surface 762, which faces the object side, is a convex surface, and an image-side surface 764, which faces the image side, is a convex surface. The object-side surface 762 has two inflection points, and the image-side surface 764 has three inflection points. Whereby, incident angle of each field of view for the sixth lens 760 can be effectively adjusted to improve aberration.

The seventh lens 770 has negative refractive power and is made of plastic. An object-side surface 772, which faces the object side, is a concave aspheric surface, and an image-side surface 774, which faces the image side, is a concave aspheric surface. The image-side surface 774 has an inflection point. It may help to shorten the back focal length to keep small in size. In addition, it may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 780 is made of glass and between the seventh lens 770 and the image plane 790. The infrared rays filter 780 gives no contribution to the focal length of the system.

In the seventh embodiment, the optical image capturing system of the seventh embodiment further satisfies ΣPP=51.7940 mm; and f1//ΣPP=0.2627, where ΣPP is a sum of the focal lengths of each positive lens. It is helpful to share the positive refractive power of one single lens to other positive lenses to avoid the significant aberration caused by the incident rays.

The optical image capturing system of the seventh embodiment further satisfies ΣNP=−123.3579 mm; and f7/ΣNP=0.0412, where ΣNP is a sum of the focal lengths of each negative lens. It is helpful to share the negative refractive power of one single lens to the other negative lenses to avoid the significant aberration caused by the incident rays.

The parameters of the lenses of the sixth embodiment are listed in Table 13 and Table 14.

TABLE 13 f = 6.7312 mm; f/HEP = 2.4; HAF = 47.5 deg Focal Radius of curvature Thickness Refractive Abbe length Surface (mm) (mm) Material index number (mm) 0 Object plane infinity 1 1^(st) lens 4.576054873 0.584 plastic 1.565 58.00 13.609 2 10.73151703 0.146 3 Aperture plane 0.000 4 2^(nd) lens 4.349729546 0.300 plastic 1.650 21.40 −78.642 5 3.901701278 0.466 6 3^(rd) lens −105.5977355 0.736 plastic 1.565 58.00 13.873 7 −7.33624907 0.600 8 4^(th) lens −12.30461992 1.093 plastic 1.565 58.00 16.081 9 −5.404219933 0.305 10 5^(th) lens −2.042065329 1.038 plastic 1.650 21.40 −39.630 11 −2.662144583 0.299 12 6^(th) lens 5.225384838 1.002 plastic 1.565 58.00 8.231 13 −40.50587392 1.179 14 7^(th) lens −5.140384905 0.683 plastic 1.583 30.20 −5.086 15 7.455490677 1.000 16 Infrared plane 0.300 BK_7 1.517 64.2 rays filter 17 plane 0.308 18 Image plane 0.021 plane Reference wavelength (d-line): 555 nm.

TABLE 14 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k 3.983741E−01 −4.897919E+01 −1.346812E+01 1.709440E+00 2.796516E+01 1.348422E+01 3.002689E+01 A4 2.913392E−03 −1.075801E−03 −4.722246E−03 −2.157240E−02 −1.142048E−02 −1.289707E−02 −1.813933E−02 A6 1.441858E−04 3.517095E−03 −1.071444E−03 −1.504717E−04 −2.380434E−03 −2.113505E−03 −1.073421E−03 A8 3.444720E−04 −6.440188E−04 5.560008E−04 6.756521E−04 1.308695E−04 6.047950E−04 −1.864017E−04 A10 −5.586964E−05 −2.956724E−04 −2.875384E−04 −2.753827E−04 −7.922573E−04 −4.718839E−04 2.914704E−05 A12 −2.288119E−05 1.964145E−04 5.202399E−05 −3.828904E−05 2.490353E−04 1.789349E−04 −3.549875E−06 A14 1.485701E−05 −3.377318E−05 3.415657E−07 3.001792E−05 −2.851243E−05 −4.586750E−05 −3.256825E−06 A16 −1.930238E−06 3.169793E−07 −1.357556E−07 −1.415328E−07 1.559500E−07 7.552034E−06 1.187434E−06 Surface 9 10 11 12 13 14 15 k 1.878477E+00 −4.254837E−01 −5.629283E−01 −1.475158E+00 4.334642E+01 −7.079531E−03 −5.361072E+00 A4 −1.091857E−02 2.799566E−02 1.213832E−02 −1.093232E−02 −8.871208E−03 −5.211838E−03 −4.787415E−03 A6 −9.800727E−04 −5.491994E−03 −2.342425E−03 1.697719E−03 2.900021E−03 1.558862E−03 4.143097E−04 A8 −1.534843E−04 1.122697E−03 5.035552E−04 −2.142729E−04 −3.845059E−04 −1.638382E−04 −2.918764E−05 A10 −3.106815E−05 −1.115266E−04 −4.841164E−05 1.249698E−05 2.474663E−05 9.868077E−06 1.306532E−06 A12 1.443849E−05 1.182262E−05 3.361279E−06 −3.643681E−07 −8.481899E−07 −3.373650E−07 −3.618409E−08 A14 −2.111326E−06 −8.161698E−07 −1.486190E−07 6.388407E−09 1.491450E−08 5.996697E−09 5.531837E−10 A16 6.795226E−08 5.681613E−08 2.219835E−09 −7.002687E−11 −1.033092E−10 −4.078697E−11 −3.615103E−12

An equation of the aspheric surfaces of the seventh embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the seventh embodiment based on Table 13 and Table 14 are listed in the following table:

Seventh embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.4946 0.0856 0.4852 0.4186 0.1699 0.8178 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 1.3235 2.2162 1.5790 1.4036 0.0218 0.1752 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.1730 5.6689 2.4355 1.85832 HOS InTL HOS/HOI InS/HOS ODT % TDT %2 10.0613 8.4321 1.3415 0.9274 1.9205 1.00662 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 2.7883 0.0000 0.0000 3.5682 0.4758 0.3546 PSTA PLTA NSTA NLTA SSTA SLTA 0.009 −0.00016 mm 0.002 mm 0.002 mm 0.004 mm 0.002 mm mm

The figures related to the profile curve lengths obtained based on Table 13 and Table 14 are listed in the following table:

Seventh embodiment (Reference wavelength: 555 nm) ARE ½(HEP) ARE value ARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.402 1.430 0.027 101.95% 0.584 244.74% 12 1.402 1.406 0.004 100.26% 0.584 240.66% 21 1.402 1.412 0.010 100.70% 0.300 470.74% 22 1.402 1.419 0.017 101.18% 0.300 472.95% 31 1.402 1.408 0.006 100.40% 0.736 191.40% 32 1.402 1.431 0.028 102.02% 0.736 194.48% 41 1.402 1.420 0.018 101.27% 1.093 129.98% 42 1.402 1.433 0.031 102.21% 1.093 131.19% 51 1.402 1.487 0.084 106.02% 1.038 143.29% 52 1.402 1.456 0.054 103.82% 1.038 140.32% 61 1.402 1.413 0.010 100.72% 1.002 140.92% 62 1.402 1.403 0.001 100.04% 1.002 139.97% 71 1.402 1.422 0.020 101.42% 0.683 208.11% 72 1.402 1.408 0.005 100.37% 0.683 205.97% ARS EHD ARS value ARS − EHD (ARS/EHD) % TP ARS/TP (%) 11 1.709 1.768 0.059 103.47% 0.584 302.72% 12 1.447 1.451 0.004 100.27% 0.584 248.45% 21 1.459 1.470 0.011 100.72% 0.300 489.91% 22 1.578 1.598 0.020 101.29% 0.300 532.77% 31 1.632 1.656 0.024 101.48% 0.736 225.12% 32 1.887 2.054 0.167 108.85% 0.736 279.17% 41 2.155 2.388 0.233 110.79% 1.093 218.57% 42 2.436 3.098 0.662 127.17% 1.093 283.58% 51 2.539 2.937 0.398 115.66% 1.038 283.03% 52 3.190 3.437 0.247 107.75% 1.038 331.25% 61 4.464 4.617 0.154 103.45% 1.002 460.69% 62 4.688 4.864 0.176 103.75% 1.002 485.27% 71 4.734 5.252 0.518 110.93% 0.683 768.47% 72 6.170 6.812 0.642 110.41% 0.683 996.84%

The results of the equations of the seventh embodiment based on Table 13 and Table 14 are listed in the following table:

Values related to the inflection points of the seventh embodiment (Reference wavelength: 555 nm) HIF211 1.0924 HIF211/HOI 0.1457 SGI211 0.1095 |SGI211|/(|SGI211| + TP2) 0.2673 HIF521 2.1002 HIF521/HOI 0.2800 SGI521 −0.7289 |SGI521|/(|SGI521| + TP5) 0.4126 HIF611 1.7227 HIF611/HOI 0.2297 SGI611 0.2145 |SGI611|/(|SGI611| + TP6) 0.1763 HIF612 3.9127 HIF612/HOI 0.5217 SGI612 0.0038 |SGI612|/(|SGI612| + TP6) 0.0038 HIF621 1.6536 HIF621/HOI 0.2205 SGI621 −0.0595 |SGI621|/(|SGI621| + TP6) 0.0560 HIF622 2.2525 HIF622/HOI 0.3003 SGI622 −0.0994 |SGI622|/(|SGI622| + TP6) 0.0902 HIF623 4.2291 HIF623/HOI 0.5639 SGI623 −0.6719 |SGI623|/(|SGI623| + TP6) 0.4013 HIF721 1.7490 HIF721/HOI 0.2332 SGI721 0.1590 |SGI721|/(|SGI721| + TP7) 0.1887

Eighth Embodiment

As shown in FIG. 8A and FIG. 8B, an optical image capturing system of the eighth embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 810, an aperture 800, a second lens 820, a third lens 830, a fourth lens 840, a fifth lens 850, a seventh lens 860, a seventh lens 870, an infrared rays filter 880, an image plane 890, and an image sensor 892. FIG. 8C is a transverse aberration diagram at 0.7 field of view of the eighth embodiment of the present application.

The first lens 810 has positive refractive power and is made of plastic. An object-side surface 812, which faces the object side, is a convex aspheric surface, and an image-side surface 814, which faces the image side, is a concave aspheric surface.

The second lens 820 has negative refractive power and is made of plastic. An object-side surface 822 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 824 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 822 and the image-side surface 824 both have an inflection point.

The third lens 830 has positive refractive power and is made of plastic. An object-side surface 832, which faces the object side, is a convex aspheric surface, and an image-side surface 834, which faces the image side, is a convex aspheric surface. The object-side surface 832 has an inflection point.

The fourth lens 840 has positive refractive power and is made of plastic. An object-side surface 842, which faces the object side, is a concave aspheric surface, and an image-side surface 844, which faces the image side, is a convex aspheric surface. The object-side surface 842 and the image-side surface 844 both have an inflection point.

The fifth lens 850 has negative refractive power and is made of plastic. An object-side surface 852, which faces the object side, is a concave aspheric surface, and an image-side surface 854, which faces the image side, is a convex aspheric surface. The image-side surface 854 has an inflection point.

The sixth lens 860 can have positive refractive power and is made of plastic. An object-side surface 862, which faces the object side, is a convex surface, and an image-side surface 864, which faces the image side, is a convex surface. The object-side surface 862 and the image-side surface 864 both have two inflection points. Whereby, incident angle of each field of view for the sixth lens 860 can be effectively adjusted to improve aberration.

The seventh lens 870 has negative refractive power and is made of plastic. An object-side surface 872, which faces the object side, is a concave surface, and an image-side surface 874, which faces the image side, is a concave surface. The image-side surface 874 has an inflection point. It may help to shorten the back focal length to keep small in size. In addition, it may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 880 is made of glass and between the seventh lens 870 and the image plane 890. The infrared rays filter 880 gives no contribution to the focal length of the system.

In the eighth embodiment, the optical image capturing system of the seventh embodiment further satisfies ΣPP=58.8575 mm; and f1/ΣPP=0.2270, where ΣPP is a sum of the focal lengths of each positive lens. It is helpful to share the positive refractive power of one single lens to other positive lenses to avoid the significant aberration caused by the incident rays.

The optical image capturing system of the eighth embodiment further satisfies ΣNP=−151.0523 mm; and f7/ΣNP=0.0333, where ΣNP is a sum of the focal lengths of each negative lens. It is helpful to share the negative refractive power of one single lens to the other negative lenses to avoid the significant aberration caused by the incident rays.

The parameters of the lenses of the sixth embodiment are listed in Table 15 and Table 16.

TABLE 15 f = 6.7652 mm; f/HEP = 2.8; HAF = 47.4999 deg Focal Radius of curvature Thickness Refractive Abbe length Surface (mm) (mm) Material index number (mm) 0 Object plane infinity 1 1^(st) lens 3.971861976 0.704 plastic 1.543 56.50 13.358 2 8.198255892 0.329 3 Aperture plane 0.026 4 2^(nd) lens 5.77169029 0.300 plastic 1.650 21.40 −44.180 5 4.713442648 0.215 6 3^(rd) lens 94.59884361 0.616 plastic 1.543 56.50 11.105 7 −6.447953968 0.557 8 4^(th) lens −8.179862942 0.829 plastic 1.565 58.00 25.453 9 −5.411402961 0.433 10 5^(th) lens −2.026486659 0.924 plastic 1.650 21.40 −101.838 11 −2.467389187 0.312 12 6^(th) lens 5.633670908 1.253 plastic 1.543 56.50 8.941 13 −33.15343005 1.113 14 7^(th) lens −5.076660311 0.722 plastic 1.607 26.60 −5.035 15 8.230543784 1.000 16 Infrared plane 0.300 BK_7 1.517 64.2 rays filter 17 plane 0.205 18 Image plane 0.017 plane Reference wavelength (d-line): 555 nm.

TABLE 16 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k 5.195598E−01 −1.128183E+01 −1.943087E+01 3.467668E−01 −5.000000E+01 1.338720E+01 1.761403E+01 A4 2.356299E−03 2.397565E−03 −1.680699E−02 −2.546780E−02 −7.060172E−03 −1.007863E−02 −2.355210E−02 A6 6.485149E−04 1.229684E−03 −2.729378E−03 −3.136590E−03 −2.003546E−03 −1.218487E−03 −9.785530E−04 A8 1.170764E−04 2.918717E−04 −2.459869E−04 1.932658E−03 −2.237902E−03 7.543922E−04 −1.852033E−04 A10 3.039274E−05 −1.491091E−04 5.676525E−04 −1.058044E−03 1.435439E−04 −7.355860E−04 −1.348843E−04 A12 6.643196E−07 −4.266383E−05 −7.384056E−05 1.268094E−04 4.255759E−04 2.634268E−04 −1.539980E−05 A14 −2.883111E−06 9.237416E−05 −1.409057E−05 4.839477E−05 −2.015694E−04 2.011329E−05 1.121679E−05 A16 1.624359E−06 −2.281995E−05 −1.202828E−05 3.364385E−06 1.861152E−05 −3.268269E−06 5.139585E−06 Surface 9 10 11 12 13 14 15 k 4.494834E+00 −2.599360E−01 −5.817157E−01 −1.432572E+00 3.780652E+01 −3.317069E−02 −5.648669E+00 A4 −1.496778E−02 2.840014E−02 1.192087E−02 −1.085707E−02 −8.701398E−03 −5.652365E−03 −5.333227E−03 A6 −1.207485E−03 −5.261084E−03 −2.232665E−03 1.702507E−03 2.912311E−03 1.558055E−03 4.182781E−04 A8 −1.928552E−04 1.084879E−03 5.252541E−04 −2.142161E−04 −3.841236E−04 −1.631492E−04 −2.906249E−05 A10 −7.621215E−05 −9.710755E−05 −4.639259E−05 1.251520E−05 2.474808E−05 9.896558E−06 1.305194E−06 A12 1.195672E−05 1.741965E−05 3.509831E−06 −3.632770E−07 −8.486325E−07 −3.366865E−07 −3.626114E−08 A14 −8.617708E−07 7.804099E−08 −1.504508E−07 6.388220E−09 1.487244E−08 5.983719E−09 5.528456E−10 A16 2.229654E−07 −1.196294E−08 −2.297951E−09 −7.540487E−11 −1.059054E−10 −4.339767E−11 −3.536156E−12

An equation of the aspheric surfaces of the eighth embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the eighth embodiment based on Table 15 and Table 16 are listed in the following table:

Eighth embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.5065 0.1531 0.6092 0.2658 0.0664 0.7566 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 1.3438 2.1381 1.5633 1.3676 0.0525 0.1645 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.3024 3.9784 3.5329 1.46352 HOS InTL HOS/HOI InS/HOS ODT % TDT %2 9.8561 8.3336 1.3142 0.8951 1.4318 1.09772 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 0.0000 0.0000 0.5599 0.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 2.7508 0.0000 0.0000 3.0221 0.4029 0.3066 PSTA PLTA NSTA NLTA SSTA SLTA 0.003 mm −0.001 mm 0.002 mm 0.002 mm 0.004 mm 0.002 mm

The figures related to the profile curve lengths obtained based on Table 15 and Table 16 are listed in the following table:

Eighth embodiment (Reference wavelength: 555 nm) ARE ½(HEP) ARE value ARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.208 1.230 0.022 101.82% 0.704 174.62% 12 1.208 1.213 0.005 100.41% 0.704 172.20% 21 1.203 1.204 0.001 100.12% 0.300 401.37% 22 1.208 1.213 0.005 100.38% 0.300 404.22% 31 1.208 1.209 0.001 100.05% 0.616 196.36% 32 1.208 1.223 0.015 101.27% 0.616 198.75% 41 1.208 1.224 0.016 101.35% 0.829 147.71% 42 1.208 1.229 0.020 101.69% 0.829 148.21% 51 1.208 1.268 0.060 104.94% 0.924 137.14% 52 1.208 1.250 0.042 103.49% 0.924 135.25% 61 1.208 1.214 0.006 100.51% 1.253 96.89% 62 1.208 1.209 0.001 100.05% 1.253 96.44% 71 1.208 1.221 0.013 101.09% 0.722 169.23% 72 1.208 1.211 0.003 100.25% 0.722 167.82% ARS EHD ARS value ARS − EHD (ARS/EHD) % TP ARS/TP (%) 11 1.847 1.974 0.127 106.89% 0.704 280.21% 12 1.525 1.538 0.013 100.84% 0.704 218.35% 21 1.203 1.204 0.001 100.12% 0.300 401.37% 22 1.365 1.369 0.004 100.29% 0.300 456.26% 31 1.419 1.422 0.004 100.27% 0.616 231.09% 32 1.631 1.699 0.068 104.16% 0.616 275.95% 41 1.841 2.007 0.165 108.99% 0.829 242.07% 42 2.105 2.538 0.433 120.58% 0.829 306.23% 51 2.228 2.585 0.358 116.06% 0.924 279.70% 52 2.886 3.141 0.255 108.85% 0.924 339.79% 61 4.406 4.546 0.140 103.17% 1.253 362.72% 62 4.757 5.029 0.272 105.72% 1.253 401.28% 71 4.793 5.361 0.568 111.86% 0.722 742.98% 72 6.060 6.698 0.638 110.52% 0.722 928.17%

The results of the equations of the seventh embodiment based on Table 15 and Table 16 are listed in the following table:

Values related to the inflection points of the eighth embodiment (Reference wavelength: 555 nm) HIF211 0.7069 HIF211/HOI 0.0943 SGI211 0.0361 |SGI211|/(|SGI211| + TP2) 0.1074 HIF221 0.8103 HIF221/HOI 0.1080 SGI221 0.0587 |SGI221|/(|SGI221| + TP2) 0.1637 HIF311 0.3368 HIF311/HOI 0.0449 SGI311 0.0005 |SGI311|/(|SGI311| + TP3) 0.0008 HIF521 1.9895 HIF521/HOI 0.2653 SGI521 −0.7223 |SGI521|/(|SGI521| + TP5) 0.4387 HIF611 1.6840 HIF611/HOI 0.2245 SGI611 0.1891 |SGI611|/(|SGI611| + TP6) 0.1311 HIF612 3.9045 HIF612/HOI 0.5206 SGI612 −0.0249 |SGI612|/(|SGI612| + TP6) 0.0195 HIF621 1.6440 HIF621/HOI 0.2192 SGI621 −0.0651 |SGI621|/(|SGI621| + TP6) 0.0494 HIF622 2.3170 HIF622/HOI 0.3089 SGI622 −0.1126 |SGI622|/(|SGI622| + TP6) 0.0824 HIF721 1.5156 HIF721/HOI 0.2021 SGI721 0.1106 |SGI721|/(|SGI721| + TP7) 0.1329

It must be pointed out that the embodiments described above are only some embodiments of the present invention. All equivalent structures which employ the concepts disclosed in this specification and the appended claims should fall within the scope of the present invention. 

1. An optical image capturing system, in order along an optical axis from an object side to an image side, comprising: a first lens having refractive power; a second lens having refractive power; a third lens having refractive power; a fourth lens having refractive power; a fifth lens having refractive power; a sixth lens having refractive power; a seventh lens having refractive power; and an image plane; wherein the optical image capturing system consists of the seven lenses with refractive power; a maximum height for image formation perpendicular to the optical axis on the image plane is denoted as HOI; at least one lens among the first lens to the third lens has positive refractive power; at least one lens among the fourth lens to the seventh lens has positive refractive power; each lens among the first lens to the seventh lens has an object-side surface, which faces the object side, and an image-side surface, which faces the image side; wherein the optical image capturing system satisfies: 1.4≦f/HEP≦10.0; 0 deg<HAF≦150 deg; and 0.9≦2(ARE/HEP)≦1.5; where f1, f2, f3, f4, f5, f6, and f7 are focal lengths of the first lens to the seventh lens, respectively; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HOS is a distance in parallel with the optical axis from the object-side surface of the first lens to the image plane; InTL is a distance from the object-side surface of the first lens to the image-side surface of the seventh lens on the optical axis; for any surface of any lens, HAF is a half of a view angle of the optical image capturing system, ARE is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis.
 2. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: PLTA≦200 μm; PSTA≦200 μm; NLTA≦200 μm; NSTA≦200 μm; SLTA≦200 μm; SSTA≦200 μm; and |TDT|<250%; where TDT is a TV distortion; HOI is a maximum height for image formation perpendicular to the optical axis on the image plane; PLTA is a transverse aberration at 0.7 HOI on the image plane in the positive direction of a tangential fan of the optical image capturing system after a longest operation wavelength of visible light passing through an edge of the aperture; PSTA is a transverse aberration at 0.7 HOI on the image plane in the positive direction of the tangential fan after a shortest operation wavelength of visible light passing through the edge of the aperture; NLTA is a transverse aberration at 0.7 HOI on the image plane in the negative direction of the tangential fan after the longest operation wavelength of visible light passing through the edge of the aperture; NSTA is a transverse aberration at 0.7 HOI on the image plane in the negative direction of the tangential fan after the shortest operation wavelength of visible light passing through the edge of the aperture; SLTA is a transverse aberration at 0.7 HOI on the image plane of a sagittal fan of the optical image capturing system after the longest operation wavelength of visible light passing through the edge of the aperture; SSTA is a transverse aberration at 0.7 HOI on the image plane of a sagittal fan after the shortest operation wavelength of visible light passing through the edge of the aperture.
 3. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: 0.9≦ARS/EHD≦2.0; where, for any surface of any lens, EHD is a maximum effective half diameter thereof, ARS is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to an end point of the maximum effective half diameter thereof.
 4. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: 0 mm<HOS≦50 mm.
 5. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: 0 deg<HAF≦70 deg; where HAF is a half of a view angle of the optical image capturing system.
 6. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: 0.05≦ARE71/TP7≦25; and 0.05≦ARE72/TP7≦25; where ARE71 is a profile curve length measured from a start point where the optical axis passes the object-side surface of the seventh lens, along a surface profile of the object-side surface of the seventh lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis; ARE72 is a profile curve length measured from a start point where the optical axis passes the image-side surface of the seventh lens, along a surface profile of the image-side surface of the seventh lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis; TP7 is a thickness of the seventh lens on the optical axis.
 7. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: 0.05≦ARE61/TP6≦25; and 0.05≦ARE62/TP6≦25; where ARE61 is a profile curve length measured from a start point where the optical axis passes the object-side surface of the sixth lens, along a surface profile of the object-side surface of the sixth lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis; ARE62 is a profile curve length measured from a start point where the optical axis passes the image-side surface of the sixth lens, along a surface profile of the image-side surface of the sixth lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis; TP6 is a thickness of the sixth lens on the optical axis.
 8. The optical image capturing system of claim 1, wherein the first lens has positive refractive power, and the second lens has negative refractive power.
 9. The optical image capturing system of claim 1, further comprising an aperture, wherein the optical image capturing system further satisfies: 0.2≦InS/HOS≦1.1; where InS is a distance in parallel with the optical axis between the aperture and the image plane.
 10. An optical image capturing system, in order along an optical axis from an object side to an image side, comprising: a first lens having refractive power; a second lens having refractive power; a third lens having refractive power; a fourth lens having refractive power; a fifth lens having refractive power; a sixth lens having refractive power; a seventh lens having refractive power; and an image plane; wherein the optical image capturing system consists of the seven lenses with refractive power; at least a surface of at least two lenses among the first lens to the seventh lens has at least an inflection point; at least one lens among the first lens to the third lens has positive refractive power; at least one lens among the fourth lens to the seventh lens has positive refractive power; each lens among the first lens to the seventh lens has an object-side surface, which faces the object side, and an image-side surface, which faces the image side; wherein the optical image capturing system satisfies: 1.4≦f/HEP≦10.0; 0<InTL/HOS<0.9; 0 deg<HAF≦150 deg; and 0.9≦2(ARE/HEP)≦1.5; where f1, f2, f3, f4, f5, f6, and f7 are focal lengths of the first lens to the seventh lens, respectively; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HOS is a distance in parallel with the optical axis between the object-side surface of the first lens and the image plane; InTL is a distance from the object-side surface of the first lens to the image-side surface of the seventh lens on the optical axis; for any surface of any lens, HAF is a half of a view angle of the optical image capturing system, ARE is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis.
 11. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: 0.9≦ARS/EHD≦2.0; where, for any surface of any lens, EHD is a maximum effective half diameter thereof, ARS is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to an end point of the maximum effective half diameter thereof.
 12. The optical image capturing system of claim 10, wherein at least a surface of at least three lenses among the first lens to the seventh lens has at least an inflection point thereon.
 13. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: PLTA≦200 μm; PSTA≦200 μm; NLTA≦200 μm; NSTA≦200 μm; SLTA≦200 μm; SSTA≦200 μm; and HOI>3.0 mm; where HOI is a maximum height for image formation perpendicular to the optical axis on the image plane; PLTA is a transverse aberration at 0.7 HOI on the image plane in the positive direction of a tangential fan of the optical image capturing system after a longest operation wavelength of visible light passing through an edge of the aperture; PSTA is a transverse aberration at 0.7 HOI on the image plane in the positive direction of the tangential fan after a shortest operation wavelength of visible light passing through the edge of the aperture; NLTA is a transverse aberration at 0.7 HOI on the image plane in the negative direction of the tangential fan after the longest operation wavelength of visible light passing through the edge of the aperture; NSTA is a transverse aberration at 0.7 HOI on the image plane in the negative direction of the tangential fan after the shortest operation wavelength of visible light passing through the edge of the aperture; SLTA is a transverse aberration at 0.7 HOI on the image plane of a sagittal fan of the optical image capturing system after the longest operation wavelength of visible light passing through the edge of the aperture; SSTA is a transverse aberration at 0.7 HOI on the image plane of a sagittal fan after the shortest operation wavelength of visible light passing through the edge of the aperture.
 14. The optical image capturing system of claim 10, wherein at least one lens among the first lens, the second lens, the third lens, the fourth lens, the fifth lens, the sixth lens, and the seventh lens is a filter, which is capable of filtering out light of wavelengths shorter than 500 nm.
 15. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: 0<IN12/f≦3.0; where IN12 is a distance on the optical axis between the first lens and the second lens.
 16. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: 0<IN67/f≦0.8; where IN67 is a distance on the optical axis between the sixth lens and the seventh lens.
 17. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: 0.1≦(TP7+IN67)/TP6≦10; where IN67 is a distance on the optical axis between the sixth lens and the seventh lens; TP6 is a thickness of the sixth lens on the optical axis; TP7 is a thickness of the seventh lens on the optical axis.
 18. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: 0.1≦(TP1+IN12)/TP2≦10; where IN12 is a distance on the optical axis between the first lens and the second lens; TP1 is a thickness of the first lens on the optical axis; TP2 is a thickness of the second lens on the optical axis.
 19. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: 0<TP4/(IN34+TP4+IN45)<1; where IN34 is a distance on the optical axis between the third lens and the fourth lens; IN45 is a distance on the optical axis between the fourth lens and the fifth lens; TP4 is a thickness of the fourth lens on the optical axis.
 20. An optical image capturing system, in order along an optical axis from an object side to an image side, comprising: a first lens having positive refractive power; a second lens having refractive power; a third lens having refractive power; a fourth lens having refractive power; a fifth lens having refractive power; a sixth lens having refractive power; a seventh lens having refractive power; and an image plane; wherein the optical image capturing system consists of the seven lenses having refractive power; a maximum height for image formation perpendicular to the optical axis on the image plane is denoted as HOI; at least a surface of each of at least three lenses among the first lens to the seventh lens has at least an inflection point thereon; each lens among the first lens to the seventh lens has an object-side surface, which faces the object side, and an image-side surface, which faces the image side; wherein the optical image capturing system satisfies: 1.4≦f/HEP≦10.0; 0<InTL/HOS<0.9; 0 deg<HAF≦150 deg; and 0.9<2(ARE/HEP)≦1.5; where f1, f2, f3, f4, f5, f6, and f7 are focal lengths of the first lens to the seventh lens, respectively; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HOS is a distance in parallel with the optical axis between an object-side surface, which face the object side, of the first lens and the image plane; InTL is a distance from the object-side surface of the first lens to the image-side surface of the seventh lens on the optical axis; HAF is a half of a maximum field angle of the optical image capturing system; for any surface of any lens, ARE is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis.
 21. The optical image capturing system of claim 20, wherein the optical image capturing system further satisfies: 0.9≦ARS/EHD≦2.0; where, for any surface of any lens, EHD is a maximum effective half diameter thereof, ARS is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to an end point of the maximum effective half diameter thereof.
 22. The optical image capturing system of claim 20, wherein the optical image capturing system further satisfies: 0 mm<HOS≦50 mm.
 23. The optical image capturing system of claim 20, wherein the optical image capturing system further satisfies: 0.05≦ARE71/TP7≦25; and 0.05≦ARE72/TP7≦25; where ARE71 is a profile curve length measured from a start point where the optical axis passes the object-side surface of the seventh lens, along a surface profile of the object-side surface of the seventh lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis; ARE72 is a profile curve length measured from a start point where the optical axis passes the image-side surface of the seventh lens, along a surface profile of the image-side surface of the seventh lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis; TP7 is a thickness of the seventh lens on the optical axis.
 24. The optical image capturing system of claim 20, wherein the optical image capturing system further satisfies: 0.05≦ARE61/TP6≦25; and 0.05≦ARE62/TP6≦25; where ARE61 is a profile curve length measured from a start point where the optical axis passes the object-side surface of the sixth lens, along a surface profile of the object-side surface of the sixth lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis; ARE62 is a profile curve length measured from a start point where the optical axis passes the image-side surface of the sixth lens, along a surface profile of the image-side surface of the sixth lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis; TP6 is a thickness of the sixth lens on the optical axis.
 25. The optical image capturing system of claim 20, further comprising an aperture an image sensor, and a driving module, wherein the image sensor is disposed on the image plane; the driving module is coupled with the lenses to move the lenses; the optical image capturing system further satisfies: 0.2≦InS/HOS≦1.1; where InS is a distance in parallel with the optical axis between the aperture and the image plane. 